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Coaster Quest<br />

THE PHYSICS AND MATHEMATICS OF AMUSEMENT PARK RIDES<br />

Physics<br />

© Copyrighted by The Center for Mathematics, Science,<br />

and Technology Education, Kutztown University of<br />

Pennsylvania. This material is based upon work supported<br />

by the National Science Foundation under Grant<br />

No. 9986753.<br />

Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation.


<strong>Dorney</strong> <strong>Park</strong>/Kutztown University<br />

Coaster Quest<br />

Introduction<br />

The Lehigh Valley is rich in tradition, culture and beauty. We are most<br />

fortunate to have a community of fine people who are dedicated to the enhancement of<br />

our quality of life. To these ends, <strong>Dorney</strong> <strong>Park</strong> and Kutztown University have<br />

collaborated in the development of an educational experience that will benefit the<br />

children of the Lehigh Valley and beyond.<br />

We call it Coaster Quest. Our goal is to provide a stimulating and challenging<br />

exploratory experience for high school students. We utilize some of <strong>Dorney</strong> <strong>Park</strong>’s best<br />

attractions in ways that promote a deeper and more profound understanding of select<br />

scientific and mathematical principles. Students are given the opportunity to examine<br />

and study relationships between the dynamics of the mechanical universe and the<br />

unique, structural features of the rides.<br />

Kutztown University of Pennsylvania is pleased once again to participate in a<br />

collaborative project that engages future teachers in serious work with leading<br />

educators and the community. For science and mathematics teachers, this represents the<br />

best of two worlds, a living classroom replete with experiential activities and a forum<br />

for examining the connections between theory and practice. For <strong>Dorney</strong> <strong>Park</strong>, this is yet<br />

another opportunity to showcase their outstanding amusement park. All who<br />

participate will examine the extraordinary structural design process that went into the<br />

construction of these fabulous rides.<br />

We extend to you the opportunity to examine our laboratory manual, review<br />

procedural aspects, and participate in our tenth annual Coaster Quest day that will be<br />

held on May 6, 2011. Well over 45,000 students from regional schools have participated<br />

in our annual Coaster Quest. With the addition of new and exciting activities, we<br />

believe that you and your students will find the day both thrilling and enlightening.<br />

Dr. Joseph S. Elias<br />

Professor of Science Education<br />

College of Education<br />

Kutztown University of Pennsylvania


Coaster Quest<br />

Table of Contents<br />

Planning Team Page i<br />

Tips for Teachers Page ii<br />

Things to Bring Page iii<br />

The Rides Page 1<br />

Apollo 2000 Page 1<br />

The Antique Carrousel Page 8<br />

The Ferris Wheel Page 13<br />

The Enterprise Page 19<br />

Revolution Page 23<br />

The Dominator Page 27<br />

The Sea Dragon Page 32<br />

White Water Landing Page 37<br />

The Scrambler Page 42<br />

The Wave Swinger Page 47<br />

Steel Force Page 52<br />

Energy Curves for Steel<br />

Force<br />

Page 61<br />

Centripetal Force and Steel<br />

Force<br />

Page 65<br />

The Talon Page 67<br />

Thunderhawk Page 75<br />

The Hydra Page 79<br />

Interpreting Graphs Page 94<br />

Possessed Page 101<br />

PA State Science and Technology<br />

Standards<br />

Page 113


Coaster Quest


Coaster Quest<br />

<strong>Dorney</strong> <strong>Park</strong>/Kutztown University<br />

Planning Team<br />

The making of an event of such monumental scope can only be<br />

accomplished when the “players” are truly dedicated to its goals. Such is the<br />

nature of our planning team. The planning process began in August of 1997. Since<br />

then, a core of science and mathematics teachers has enthusiastically participated<br />

in all phases of development. The professional staff of <strong>Dorney</strong> <strong>Park</strong> has graciously<br />

opened their doors, extending their guidance and technical support to those who<br />

developed the laboratories. One park professional likened it to a magician<br />

“revealing” well-kept secrets. The faculty, students, and administrators of<br />

Kutztown University have made the commitment of their time, energy and<br />

enthusiasm. Our goal has been and always will be academic excellence. We<br />

recognize the value of Coaster Quest as an instrument befitting this goal. The<br />

combined efforts of all represent the true spirit of education and service.<br />

Acknowledgment<br />

Mr. Richard Button<br />

Mr. Patrick Callahan<br />

Dr. Kathleen Dolgos<br />

Dr. David Drummer<br />

Dr. Joseph Elias<br />

Dr. Deborah Frantz<br />

Mr. Glenn Frey<br />

Mr. Joseph Greene<br />

Mr. Robert Guigley<br />

Mr. Keith Koepke<br />

Mr. William Landis<br />

Dr. Neal Shea<br />

Mrs. Brenda Snyder<br />

Mr. Jeffrey Wetherhold<br />

Mr. Brent Ohl<br />

Ms. Maggie Woodward<br />

Mr. Gerry Farnsworth<br />

Kutztown University of Pennsylvania<br />

Delaware Regional School District<br />

Kutztown University of Pennsylvania<br />

Kutztown Area School District<br />

Kutztown University of Pennsylvania<br />

Kutztown University of Pennsylvania<br />

Northwestern Lehigh School District<br />

<strong>Dorney</strong> <strong>Park</strong> of Allentown<br />

Reading Area School District<br />

<strong>Dorney</strong> <strong>Park</strong> of Allentown<br />

Allentown School District<br />

Kutztown University of Pennsylvania<br />

Kutztown University of Pennsylvania<br />

<strong>Park</strong>land School District<br />

East Penn School District<br />

Upper Perkiomen School District<br />

<strong>Park</strong>land School District<br />

And<br />

To the many graduate students of the Kutztown University of Pennsylvania who<br />

contributed to the development of this manual.<br />

i


Coaster Quest<br />

Tips for Teachers<br />

To help make your day at the park more enjoyable, we have created a list of<br />

“tips for teachers.” Hopefully, this list will guide you through the pre-visit<br />

planning stage and answer some of your questions.<br />

<br />

<br />

<br />

<br />

<br />

<br />

Please don't forget your equipment, supplies and laboratory manuals. You may find<br />

that a camcorder might be functional in a variety of ways. Perhaps you wish to discuss<br />

the dynamics of the rides as a review, incorporate them within a laboratory practical,<br />

use as introductory preparation for next year’s trip to the park.<br />

You and your students should decide on which of the many rides you want to explore.<br />

Carefully peruse the complete list of activities and find those rides that will best benefit<br />

your students.<br />

Some rides may take more time than others to complete. You may find it necessary to<br />

ride several times on some of the rides in order to collect good data.<br />

As much as is feasible, introduce to the students the concepts to be studied and rides<br />

that you have chosen during the weeks leading up to the event. Plan time in class for<br />

calculations and analysis during the days following the experience.<br />

Each teacher needs to decide how the students from his/her school will complete the<br />

data collection sheets, and any other information, that her/ his students may need. We<br />

recommend that teachers in charge advise students who may be fearful of some rides,<br />

that riding is optional and not mandatory.<br />

Kutztown University students will serve as general assistants to the teachers. They will<br />

be stationed at each listed ride and the reserved pavilion from 10:00 AM until 3:00<br />

PM. Follow the park map to the pavilion site and look for the Coaster Quest banner.<br />

Inform your students that they may ask the university students any questions related to<br />

the event with the exception of specific questions that may be contrary to your<br />

objectives.<br />

Further information may be obtained by contacting:<br />

Mr. Bernie Bonuccelli <strong>Dorney</strong> <strong>Park</strong> (610)395-3724<br />

bbonuccelli@dorneypark.com<br />

Dr. Joseph Elias Kutztown University (610) 683-4762<br />

of Pennsylvania<br />

elias@kutztown.edu<br />

ii


Coaster Quest<br />

Things to Bring<br />

To make your day at the park as functional and enjoyable as possible we<br />

suggest that you arrange to bring some or all of the items listed below:<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

tickets for you, your students and your chaperones<br />

copies of the activities that you and your students plan on doing<br />

stopwatches<br />

calculators<br />

clipboards<br />

paper and pencils<br />

masking tape<br />

protractors<br />

accelerometers<br />

inclinometers<br />

CBL (calculator based laboratory) if you have them and low range sensors for<br />

acceleration<br />

appropriate clothing with a change of clothing<br />

sunscreen, hats, raincoats<br />

money for food, drinks or phone<br />

measuring tape or string<br />

backpacks or plastic bags to keep laboratory manuals and equipment dry and<br />

together<br />

a good reserve of energy and enthusiasm for exploration<br />

<strong>Dorney</strong> <strong>Park</strong> Information<br />

For general information call (800) 551-5656<br />

(610) 395-3724<br />

Group Sales Information (610) 395-2000<br />

or<br />

Bernie Bonuccelli at 1(800) 551-5656 with any specific questions<br />

about ticket sales for Coaster Quest.<br />

or<br />

visit our website: www.dorneypark.com<br />

Thank you.<br />

iii


Apollo 2000<br />

Introduction:<br />

Rotational motion is a topic in physics that looks at<br />

objects that rotate or revolve around a point. This point is<br />

called the point of rotation. These objects have many<br />

properties associated with them. Two of these properties are angular velocity and<br />

centripetal acceleration. You will be using two different techniques to calculate<br />

centripetal acceleration. You will then be asked to compare the two methods. You will<br />

also graph the relationship between linear velocity, centripetal acceleration and the<br />

radius. Conceptual questions pertaining to your perceptions of speed and acceleration as<br />

you are riding the Apollo 2000 are at the end of the laboratory.<br />

Apparatus:<br />

stopwatch, calculator, inclinometer<br />

Procedure:<br />

Look for the Coaster Quest sign or any position to the right of the entry area of the<br />

ride for a good place to stand when taking the following measurements. This will<br />

provide a clear point of observation when doing the off ride data taking.<br />

1. Use a stopwatch to measure the time that it takes for the ride to rotate five (5) times<br />

when at full speed.<br />

t = ____________________ sec<br />

2. Calculate the time that it takes for one rotation.<br />

T =<br />

t<br />

5<br />

_________________sec<br />

3. The angular velocity, , is the angle that is swept out over a period of time of a<br />

rotating object. Calculate the angular velocity. Remember one rotation is 2<br />

radians angular distance.<br />

= __________________ rad/sec<br />

1


Apollo 2000<br />

4. When the ride is in full operation, the arms are oscillating inward and outward. Use<br />

the inclinometer to find the minimum angle and maximum angle of the arms with<br />

respect to the vertical (dashed line) as shown below. Hold the inclinometer as<br />

shown.<br />

max<br />

min<br />

4.73 meters<br />

8.4 meters<br />

across center<br />

Inclinometer<br />

Inclinometer<br />

min = ___________________degrees<br />

max = ___________________degrees<br />

NOTE: If you are using a PASCO or CENCO inclinometer, then you need to subtract<br />

from 90 to get the desired angle because they are designed to take angle measurements<br />

with respect to the horizontal.<br />

5. Examine the diagram above. On it or the rear of this sheet, sketch and apply your<br />

trigonometric rules to calculate the radius of motion of the car when it is at its<br />

maximum and minimum positions. You will be using your trigonometric skills to<br />

do this. Treat the 4.73 meters as the hypotenuse and add the opposite side of the<br />

triangle to the radius of the ride center.<br />

radius at minimum angle = rmin = ___________________ meters<br />

radius at maximum angle = rmax = __________________ meters<br />

6. By finding the radius of curvature at these two locations we can find the linear<br />

speed that you are traveling by using the appropriate equation. Calculate the linear<br />

velocity at the minimum position and maximum position. This can be found by<br />

actual distance (circumference) calculations but you may find your linear/rotational<br />

conversion easier by using V= r.<br />

linear velocity at minimum radius = vmin = _________________ m/sec<br />

linear velocity at maximum radius = vmax = _______________ m/sec<br />

2


Apollo 2000<br />

7. Whenever an object is moving in a curved path, there is acceleration applied to that<br />

object toward the center of the curve. That acceleration, which causes an object to<br />

follow that curved path, is called centripetal acceleration. You are going to find the<br />

centripetal acceleration of yourself caused by the rotational motion of the ride.<br />

Calculate the centripetal acceleration using the values of velocity that you just<br />

calculated.<br />

centripetal acceleration at vmin = ac(min) = __________________ m/sec 2<br />

centripetal acceleration at vmax = ac(max) = _________________ m/sec 2<br />

8. Complete the table by using the same equations and methods that you used in sections<br />

5 – 7. By completing the table, you will be graphing the relation of velocity to the<br />

radius and the centripetal acceleration to the radius.<br />

Complete the table:<br />

ANGLE<br />

(degrees)<br />

RADIUS<br />

(meters)<br />

VELOCITY<br />

(m/sec)<br />

CENTRIPETAL<br />

ACCELERATION<br />

(m/sec 2 )<br />

min<br />

1 <br />

2<br />

max<br />

3 <br />

4<br />

max<br />

max<br />

3


Apollo 2000<br />

9. Make a graph of centripetal acceleration ac, versus radius, r, by using the coordinate<br />

axis below. You will have to scale the axis yourself, so do so appropriately.<br />

centripetal<br />

acceleration<br />

(m/sec 2 )<br />

Graph of ac versus r.<br />

radius (meters)<br />

10. Make a graph of linear velocity, v, versus radius, r by using the coordinate axis<br />

below. You will have to scale the axis yourself, so do so appropriately<br />

velocity<br />

(m/sec)<br />

Graph of v versus r<br />

radius (meters)<br />

4


Apollo 2000<br />

Do the graphs in questions 9 and 10 represent a linear, quadratic, or inverse<br />

relationship?<br />

<br />

How can you be sure it is linear? Include any equations that created the data<br />

you graphed.<br />

Finding maximum and minimum centripetal acceleration<br />

by using force vectors<br />

11. Another method of finding centripetal accelerations is by using vectors. Vectors<br />

are the arrows shown below which show size and direction of particular values.<br />

Calculate the maximum and minimum centripetal accelerations using the<br />

following diagram and the values you found for the maximum and minimum<br />

angle. As before, the dashed line is vertical!<br />

<br />

FN<br />

<br />

Fc<br />

FW = mg<br />

Equation to use<br />

F<br />

F<br />

N<br />

N<br />

cos<br />

mg<br />

mg<br />

FN<br />

, and<br />

cos<br />

sin<br />

ma<br />

mgsin<br />

ma<br />

cos<br />

g tan<br />

a<br />

c<br />

c<br />

c<br />

centripetal acceleration at min = ac(min) = ___________________ m/sec 2<br />

centripetal acceleration at max = ac(max) = ___________________ m/sec 2<br />

5


Apollo 2000<br />

12. Collect data from three other lab groups and put the values into the table provided<br />

for you. When working on real world data, it is always best to get multiple values<br />

for each measurement. This helps find and eliminate random error in lab work.<br />

Comparison table:<br />

Answers from Procedure #5-7 Answers from Procedure #11<br />

GROUPS<br />

CENTRIPETAL<br />

ACCELERATION<br />

CENTRIPETAL<br />

ACCELERATION<br />

CENTRIPETAL<br />

ACCELERATION<br />

CENTRIPETAL<br />

ACCELERATION<br />

a c(min)<br />

(m/sec 2 )<br />

a c(max)<br />

(m/sec 2 )<br />

a c(min)<br />

(m/sec 2 )<br />

a c(max)<br />

(m/sec 2 )<br />

YOUR<br />

GROUP<br />

1<br />

2<br />

3<br />

Analyze the accuracy and precision of the data of the four laboratory groups by<br />

comparing the groups' data in the column to each other.<br />

Next, analyze the accuracy and precision of the data by comparing the four sets of<br />

answers collectively in problem #12.<br />

6


Apollo 2000<br />

Concept Questions<br />

1. How do you perceive the speed of the ride when you are swinging outward?<br />

2. How do you perceive the speed of the ride when you are swinging inward?<br />

3. When the car is at its maximum angle, why don't you feel as if you are going to<br />

fall out?<br />

4. Does the change in radius have anything to do with the angular velocity? Linear<br />

velocity? Centripetal acceleration?<br />

7


The Antique Carrousel<br />

The Physics of Just Going in Circles<br />

Introduction:<br />

Sometime between 1918 and 1925 W. H. Dentzel built<br />

a classic carrousel that <strong>Dorney</strong> <strong>Park</strong> obtained in 1995. While<br />

simple, the carrousel can demonstrate many basic and advanced<br />

concepts of circular motion.<br />

In this lab, you will progress from simple to more<br />

advanced computations on curvilinear measurement.<br />

<br />

<br />

<br />

Part One will address basic tangential speed measurements.<br />

Part Two will take you through a series of centripetal accelerations and lastly<br />

Part Three will have you analyze the system through angular measurements.<br />

Apparatus:<br />

Stopwatch, calculator, inclinometer<br />

Data Table and Measurements:<br />

In order to do all parts of this lab, several measurements will be needed. In the<br />

blanks below, measure and record the values indicated:<br />

1. Time for one revolution: ____________________<br />

(Pick a point on the carrousel and time 3 complete revolutions. Divide this by 3<br />

for a more accurate single revolution time.)<br />

2. Angle reading for the inclinometer.<br />

(Be careful of the zero degree point. Hold your inclinometer vertically against<br />

the upright bar on the horse and read values before and after rotation starts. The<br />

angle is the change in these values from the rest angle to the angle it reaches<br />

when in motion. You must do this as the bar on the horse is not vertical!)<br />

Angle 1 change (inner row)________<br />

Angle 3 change (third row)________<br />

Angle 2 change (second row)_________<br />

Angle 4 change (outer row) _________<br />

8


The Antique Carrousel<br />

Part One<br />

Basic Rotational Motion<br />

The analysis of rotational motion in the basic sense uses the general equation:<br />

V=D/T where D is the distance covered by the horse and T is the time to complete one<br />

revolution (a period). D is the circumference of the ring where the horse is located and is<br />

found by 2 R, where R is the radius of the horse’s ring (row). Find the velocities of the<br />

horses from the inner to outer rows:<br />

1. V1= 2* meters / T=_______________________<br />

(5.8 meters is the radius of the inner row of horses)<br />

2. V2= 2*meters / T=_______________________<br />

(this row radius is 6.6 meters)<br />

3. V3= 2* meters / T=_______________________<br />

4. V4= 2* meters / T=_______________________<br />

5. As you observe the motion of the horses, which appear to be going the fastest?<br />

6. How does this compare to the calculated values above?<br />

7. As you ride the horses, what factors make you feel like you are moving?<br />

8. Compare these factors with the speeds you found above.<br />

9


The Antique Carrousel<br />

Part Two<br />

Accelerations<br />

As you ride the carrousel, you may notice a different “feel” between the inner and<br />

outer horse row. This is due to the different speeds and accelerations you experience.<br />

The human body is a good accelerometer.<br />

<br />

In which direction do you feel you are accelerating and on which horses is this the<br />

most noticeable?<br />

______________________<br />

The general equation for centripetal acceleration is a=V 2 /R. (Note that V and R vary<br />

as we go from the inner to outer ring of horses. Find the values for the four horse rows<br />

below:<br />

a1=_______________<br />

a2=___________________<br />

a2=_______________<br />

a4=___________________<br />

<br />

Do these values match what you felt on the ride?<br />

_______________________<br />

We can double-check these values by using the inclinometer data. Since the<br />

inclinometer you used shows the net angle between the gravitational and centripetal<br />

acceleration components, we can show ac =g * tan In the space below, compute the<br />

values for the accelerations of the 4 rows of horses using the angles you measured and<br />

tangent equation.<br />

a1=_______________<br />

a3=_______________<br />

a2=___________________<br />

a4=___________________<br />

On the axes below, graph the values for your accelerations (found above) verses the<br />

radius. What relationship is this? Start your graph with zero and scale (R) and (a)<br />

carefully.<br />

a<br />

R<br />

10


The Antique Carrousel<br />

Part 3<br />

Angular computations<br />

Many people have trouble understanding the rotational components of motion. They<br />

are actually simple to do. Consider the following:<br />

<br />

Which row of horses takes the longest to go around one revolution?<br />

OK, a simple question, they all take the same time. While the velocities differ (as seen<br />

in Part One), the time and angle they cover are all the same. We call this measure the<br />

angular velocity. If we have the period T from the data we took in the beginning:<br />

radians)/T (seconds).<br />

<br />

What is the angular velocity for the carrousel?<br />

<br />

<br />

This value is the same for all horses, but the tangential velocity differs with radius,<br />

R. In general, the rotational measure times radius gives the tangential component. We<br />

find V=*R.<br />

For example V1=5.8 meters.<br />

<br />

How does the angular acceleration compare to angular velocity?<br />

If we start with ac=V 2 /R, and substitute V=R, we prove ac = *R.<br />

11


The Antique Carrousel<br />

As you see, there is a linear relationship between acceleration, a, and radius, R.<br />

Graph this relationship below using the value for you found on the previous page.<br />

a<br />

0 2 4 6 8 meters<br />

<br />

How does this graph compare with the data you found in Part Two?<br />

<br />

Are angular methods easier for some calculations than others?<br />

12


The Ferris Wheel<br />

Observations:<br />

The Ferris Wheel is a wonderful experience of vertical circular motion.<br />

1. Describe the feelings you would experience as you move around in<br />

the circle. Compare what you feel at the top and bottom of the ride;<br />

also compare your feelings on the way up and on the way down.<br />

Activity 1<br />

Calculating the magnitude of the linear velocity and centripetal acceleration<br />

Part (a)<br />

Observe the ride and measure the time for a gondola to repeat one full trip around the<br />

wheel. The time for one complete rotation is called the Period and indicated by the letter T.<br />

Make sure that the ride is in the midst of a full rotation (i.e. it is loaded and will not stop to pick<br />

up or discharge passengers), gather data for at least 3 different trials and find the average period.<br />

The distance traveled in one rotation is the circumference of the circle (2R). Using the radius<br />

indicated, calculate the velocity from:<br />

v = 2 R/t<br />

Data Chart for Calculating Magnitude of Velocity and Centripetal Acceleration Radius<br />

of Wheel = 12.3 m (40 ft)<br />

One Rotation Trial 1 Period(s) Trial 2 Period(s) Trial 3 Period(s ) Average Period(s)<br />

Velocity (m/s)<br />

Acceleration (m/s/s)<br />

Circular motion results from an acceleration directed towards the center of the circle (centripetal<br />

acceleration). Find the acceleration using:<br />

Centripetal acceleration = velocity squared divided by radius<br />

or<br />

aC = v 2 /r<br />

See Data Chart for Activity 1<br />

13


The Ferris Wheel<br />

Activity 2<br />

Determining the forces acting on a rider at key points<br />

To find the force required to keep you moving in this circle, according to Newton’s Second Law<br />

of Motion, you need to multiply your mass by this acceleration.<br />

Centripetal Force = mass times centripetal acceleration<br />

or<br />

FC = m aC<br />

If mass is in kg and acceleration is in m/s/s, then the unit for force is a Newton (symbol N)<br />

Data Chart for Finding Centripetal Force<br />

Your mass (kg) = _______<br />

Your Weight (N) = m * 9.8 m/s/s = _______<br />

Hint:<br />

To find your mass in kg, you may find it useful to know that the weight of a 1 kg mass on earth is<br />

approximately 2.2 pounds.<br />

velocity (m/s)<br />

Radius of Wheel<br />

(m)<br />

12.3<br />

Acceleration<br />

(m/s/s)<br />

Centripetal<br />

Force (N)<br />

14


The Ferris Wheel<br />

Part (b)<br />

The centripetal force will be the same value throughout the ride. However, the forces<br />

that combine to create the centripetal force change as the position on the circle changes. At all<br />

positions on the ride the forces add to give a total force towards the center of the wheel.<br />

Seat Force<br />

Fs<br />

A<br />

Weight Fg<br />

Seat<br />

Force Fs<br />

SeatBack<br />

Force FB<br />

Seat Back<br />

Force FB<br />

Seat Force Fs<br />

Weight<br />

Fg<br />

D<br />

B<br />

Weight<br />

Seat<br />

Force Fs<br />

Fg<br />

C<br />

Weight<br />

Fg<br />

Position A - The seat force and the weight are in opposite directions. The weight must be larger<br />

than the seat force to give a total downward force.<br />

FS = FW - FC<br />

Position B - The vertical seat force and the weight are in opposite directions and are of the same<br />

magnitude since the total must add to a force in the direction toward the center of the circle. This<br />

force acts on the rider through friction with the seat or through the back of the seat.<br />

FS = FW<br />

15


The Ferris Wheel<br />

Position C - The seat force and weight are in opposite directions. The seat force must be larger<br />

than the weight to give a total force that is upward.<br />

FS = FW + FC<br />

Position D - The vertical seat force and the weight are in opposite directions and are of the same<br />

magnitude since the total must add to a force in the direction toward the center of the circle. This<br />

force acts on the rider through friction with the seat or through the back of the seat.<br />

FS = FW<br />

Using the data calculated in previous activities, find the magnitude of the vertical seat force at<br />

each of the 4 locations.<br />

If mass is in kg and acceleration is in m/s/s, then the unit for force is a Newton (symbol N).<br />

Data Chart for Finding Seat Force<br />

Position<br />

A<br />

C<br />

Fw (N)<br />

Your Weight<br />

Vertical F C (N)<br />

From Activity 2a<br />

Fs (N)<br />

Seat Force<br />

Position<br />

Fw (N)<br />

Your Weight<br />

Vertical F C (N)<br />

B 0<br />

D 0<br />

Fs (N)<br />

Seat Force<br />

Part (c)<br />

Force factors give an indication of what the rider experiences on the ride. In a vertical circle, the<br />

force factor (FF) is defined as the ratio of the forces you feel to the force of your weight:<br />

Force Factor = Seat Force/Weight<br />

or<br />

FF = Fs/Fw<br />

The resulting number is often referred to as a “g” force, indicating how the force you feel<br />

compares to your weight. One “g” means that the forces you feel match your weight. This is<br />

what you normally experience. Two g’s mean that the force you feel is twice your weight and<br />

many people would indicate that they feel “heavier.”<br />

Use the data from Activity 2b and predict the “g” forces acting on you through the four<br />

curves:<br />

16


The Ferris Wheel<br />

Activity 2c<br />

Data Chart for Predicting Force Factors<br />

Location<br />

A<br />

B<br />

C<br />

D<br />

Fs (N)<br />

Seat Force from 2b<br />

Fw (N)<br />

Your Weight<br />

Force Factor<br />

Activity 3<br />

Measuring “g’s”<br />

Someone in your group needs to ride the Ferris Wheel. Using your vertical<br />

accelerometer (long tube), measure the g's at the four locations being studied. If possible, take<br />

three runs so that you can average your data. Remember that 1 g means that you feel forces<br />

equal to your weight, 2 g’s mean that you feel forces that are double your weight, etc. To<br />

measure “g” forces, hold the accelerometer parallel to your body (perpendicular to the floor).<br />

Carefully observe the accelerometer through one complete rotation and record your best<br />

approximation of the reading at the four points of interest.<br />

Data Chart for Measurement of “g” Forces<br />

Location A Trial 1 g force Trial 2 g force Trial 3 g force<br />

Average “g”<br />

force<br />

Location B Trial 1 g force Trial 2 g force Trial 3 g force<br />

Average “g”<br />

force<br />

Location C Trial 1 g force Trial 2 g force Trial 3 g force<br />

Average “g”<br />

force<br />

Location D Trial 1 g force Trial 2 g force Trial 3 g force<br />

Average “g”<br />

force<br />

17


The Ferris Wheel<br />

Questions for Analysis:<br />

1. Compare your calculated (predicted) force factors with the “g” forces measured on the ride.<br />

2. Where is the “g” force largest? Explain.<br />

3. Where is the “g” force smallest? Explain.<br />

4. Describe what happens to the “g” forces as you complete one full rotation on the Ferris<br />

Wheel.<br />

5. Would it be possible to design a Ferris Wheel ride where the passengers feel “weightless” at<br />

some point of the ride? Explain your reasoning.<br />

6. Explain the effects of changing the radius of the Ferris Wheel while keeping the speed of the<br />

ride the same. Describe the effects for both a larger and smaller radius.<br />

7. Explain the effects of changing the speed of the Ferris Wheel while keeping the radius of the<br />

wheel the same.<br />

18


The Enterprise<br />

GOING IN CIRCLES<br />

Introduction:<br />

The Enterprise is a good ride to experience and measure what<br />

people call “g's of force.” What they are actually measuring are the<br />

forces a body experiences as compared to the standard contact force<br />

of mg, which we experience in equilibrium. When contact forces accelerate a body, it is<br />

natural to compare the sensation and value to mg, thus the ratio of the force on a body to<br />

mg gives rise to “g's of force.” When standing or sitting with no acceleration, the contact<br />

force on our body = mg, and we experience a “g” value of mg/mg = 1.<br />

Objective:<br />

In this lab you will compare calculated "g" values of force of your experience with<br />

force meter values as measured on the Enterprise ride.<br />

Procedure<br />

Part I: Theoretical values<br />

During this ride you will be able to experience and measure “g” values for three<br />

different situations: moving in a horizontal circle, at the top of a vertical circle, and at the<br />

bottom of a vertical circle.<br />

Place all responses on the data/calculation tables that can be found within the<br />

laboratory.<br />

Using the diagrams below, write the equation for the net force on the rider. In the<br />

first two cases, it is the net vertical force, in the third case it is the horizontal force.<br />

Based on the diagrams, fill in the blanks on the data table, and then solve for the contact<br />

force Fs.<br />

19


The Enterprise<br />

Part I: Theoretical Results<br />

Fill in the blanks based on the diagrams.<br />

Diagram A Diagram B Diagram C<br />

F net = ______ - mg F net = F s + ______ F net = ______<br />

Newton's Second Law says F net = _______<br />

Finally, solving for the contact force F s<br />

Bottom Top Horizontal<br />

F s = ma + ___ F s = ____ - mg F s = ____<br />

Part II: The Experience<br />

To do this part you must go on the ride.<br />

When you are on the ride, sit on your hands, if possible, so you can better feel the<br />

force of the seat on your body. It may also be beneficial to shut your eyes at the key<br />

points of the ride so your sensations are not biased.<br />

As the ride commences take note of the push of the seat on your body, and try to<br />

compare it to the 1g feeling of the seat when you are first strapped in.<br />

After the ride is over, record on your data table whether the g's are greater, less<br />

than, or equal to 1 at each of the key positions.<br />

g values >,


The Enterprise<br />

Part III: Numerical<br />

1. Before going on the ride, you will need the centripetal acceleration of the<br />

ride at top speed by using the period and radius. The radius is taken from<br />

the blueprints and is 8.5 m. This is on your data sheet.<br />

For you to measure the period, you must climb the hill a bit to get a good<br />

view of the ride. Choose a rider or car that is easily identified. Wait until the<br />

ride is at full speed (you can tell by the sound) and time. (two revolutions).<br />

Calculate the period, which is the time for one revolution. Car # 5 is marked<br />

with a red spot.<br />

1. r = 8.5 meters<br />

Number of revolutions Total time Time for one revolution<br />

_________ ________ ____________<br />

2. Calculate the centripetal acceleration using a c = 4 2 r / T 2<br />

a c = 4 2 r / T 2<br />

a c = _____ / _____ = ____________<br />

number substitutes<br />

answer<br />

3. Now you are ready to record the “g” values by taking a force meter on<br />

the ride. Record the readings in a horizontal circle, at the top of the<br />

loop and at the bottom of the loop.<br />

Force meter readings:<br />

a. Full speed in a horizontal circle: __________________<br />

b. At the top of the vertical loop: __________________<br />

c. At the bottom of the vertical loop: __________________<br />

21


The Enterprise<br />

4. Since the force factor F f is a ratio of F s to mg, the equations in Part I<br />

become:<br />

a. Horizontal circle: F f = F s /mg = ma/mg = a/g<br />

b. Top of loop: F f = F s /mg = (ma -mg)/mg = a/g - 1<br />

c. Bottom of loop: F f = F s /mg = (ma + mg)/mg = a/g +1<br />

Calculate the predicted force factor value for each situation. The value of (a) is the<br />

centripetal acceleration and (g) is 9.8 m/s 2 on earth.<br />

Horizontal circle : F f = F s /mg = ma/mg = a/g = ______/_______ = _______<br />

Top of loop: F f = F s /mg = (ma -mg )/mg = a/g – 1 = ______/______ -1 = _______<br />

<br />

Bottom of loop: F f = F s /mg = (ma + mg)/mg = a/g +1 = _____/______ + 1 = _______<br />

Conclusion:<br />

Do the “g” values recorded compare reasonably well with those calculated from the<br />

centripetal acceleration? Support your answer.<br />

Conclusion: ______________________________________________________________<br />

_________________________________________________________________________<br />

_________________________________________________________________________<br />

_________________________________________________________________________<br />

22


Revolution<br />

The Revolution is a unique and exciting ride that combines two of the most<br />

frequently discussed motions in physics, pendulum and rotational. As the ride picks<br />

up speed the passengers are set into these two motions simultaneously, producing<br />

an unusual sensation of motion not experience in daily life. As you watch this ride<br />

you will take time measurements involving both the pendulum and rotational motions<br />

then do some calculations to determine the amount of force acting on the riders<br />

and compare the pendulum motion with that of a simple pendulum.<br />

Revolution<br />

The ride consists of a large, vertical beam that is swung back and forth like<br />

a simple pendulum. At the bottom of the beam, a large circular ring type of<br />

arrangement is attached. The riders sit along the outer rim of the ring. As the<br />

pendulum swings, the ring rotates. You will measure the period of oscillation of the<br />

vertical beam and the period of the circular motion of the ring.<br />

23


Revolution<br />

DATA: Length of the vertical beam: L= 7.25 m. (added dimension is 10.24 meters)<br />

Radius of the ring: r= 4.26 meters<br />

The Theory<br />

A. The Pendulum<br />

As you may recall from your physics class, a simple pendulum consist of a mass<br />

hanging at the end of along string or rod. The period of the motion is the time<br />

required to swing through one complete cycle from point A to point B and back to<br />

A. See the diagram below.<br />

A<br />

B<br />

The period T is given by<br />

T = 2<br />

Where L is the length of the pendulum and ‘g’ is the acceleration due to gravity.<br />

G = 9.90 m/s 2<br />

B. Centripetal Force<br />

24


Revolution<br />

Whenever an object of mass ‘m’ is moving on a circular path of radius ‘r’ with a<br />

speed ‘v’ there is a centripetal force ‘F’ acting on the object and it is given by the<br />

formula:<br />

F =mv 2 / r<br />

This force is always directed toward the center of the circle. The passengers on<br />

the ride are seated around the circumference of a circle. As the ring rotates, the<br />

passengers feel a centripetal force given by equation number 2.<br />

V =<br />

Where T is the period (time to complete one cycle).<br />

The Procedure<br />

A. Pendulum Motion<br />

1. When the ride begins, use a stopwatch to measure the time it takes for the<br />

system to complete 4 cycles of the pendulum type motion. From this time,<br />

calculate the time for one cycle (the period T).<br />

Time for 4 cycles = ________________________________seconds<br />

T = ____________________________________________seconds<br />

2. Solve equation number 1 for the length L of a simple pendulum that has the<br />

same period as the revolution pendulum. Compare this length to the length of<br />

the actual vertical beam.<br />

B. Rotational Motion<br />

25


Revolution<br />

3. When the ride begins to move, measure the time it takes for the passengers<br />

to complete 4 rotations. From this time, calculate the time required for one<br />

rotation. From this time and equation number 3, calculate the speed ‘v’ of<br />

the riders. Using equation number 2 to calculate the force on a rider (use<br />

your own mass ‘m’)<br />

Time for 4 cycles = __________________________seconds<br />

T = _______________________________________seconds<br />

V = ______________________________________m/s<br />

F = ______________________________________N<br />

4. From the force ‘N’, calculate the ratio of the force ‘F’ to the weigh ‘mg’.<br />

This would be the so-called ‘g’ force acting on the rider.<br />

F /mg = ________________________________<br />

26


If there was one scientist who would love modern amusement parks, it<br />

would probably be Galileo Galilei. The freefall condition he studied so<br />

carefully richly experience in this modern day environment. Advanced<br />

technology had made experiencing freefall not only safe, but exciting as<br />

well. We will analyze freefall in this laboratory activity.<br />

Dominator at <strong>Dorney</strong> <strong>Park</strong> is two different rides built on one common<br />

tower. One side launches you upward at 22 m/s and allows you almost<br />

four seconds of freefall condition while you decelerate and return to the<br />

launch point. The other side lifts you to 52 meters and launches you<br />

downward at nearly 18 m/s where YOU bounce on an air cushion to<br />

almost half of the initial height. The two different versions of the ride will be used to analyze<br />

two different aspects of motion. Launch side will<br />

look at basic kinematics and accelerated motion while the Drop side will<br />

examine momentum/impulse and work/energy conditions.<br />

Launch Side and Kinematics: To study the basic kinematics of Dominator,<br />

you will need to observe the following details:<br />

Sketch Dominator and mark in<br />

relative positions and time data.<br />

Time of launch acceleration_______ seconds (observe the bodies of riders<br />

to see when acceleration begins and ends)<br />

Time of freefall condition _______________ seconds (observe between<br />

acceleration and deceleration periods)<br />

Time of deceleration ____________________ seconds<br />

(watch when arms and legs drop)<br />

When you ride, you may also take acceleration data with your force meter<br />

and log them below:<br />

launch acceleration force reading ____________<br />

freefall acceleration force reading ____________<br />

deceleration force reading __________________<br />

With the motion data collected, you will be able to find the following values:<br />

Since in a frictionless environment (which we will assume since air drag is minimal)<br />

V up =-V down V = V down - V up = 2 V up = g T freefall<br />

27


Since we are on Earth, g = 9.8 m/s/s downward and the delta V value is negative (your<br />

instructor may ask you to show that!), we can find the Velocity by using the previous equation.<br />

Vup = g * _______________=______________ m/sec<br />

With this value, we can find the acceleration and deceleration you experience at the start and<br />

end of the ride. Note you may get a 4g reading, but the calculations below will be much less.<br />

Don’t worry; trust the numbers, differences will be discussed in question #3.<br />

Aup= Vup / Tup= _____________m/s/s / _______________sec.= ________________m/s/s<br />

Adown=Vdown/Tdown=Vup/Tup=______________m/s / ____________sec.=__________m/s/s<br />

Convert these two accelerations to g’s or Force Factor readings by dividing by 9.8 m/s/s.<br />

FFup=Aup/9.8m/s/s=_____________ “g’s”, FFdown=Adown/9.8m/s/s=___________”g’s”<br />

Questions<br />

1. How do the force factors or “g” readings compare? What are sources of error?<br />

2. What is wrong with the advertising statement?<br />

Riders reach speeds of nearly 50 mph almost instantly after takeoff then experience<br />

negative gravity before they plummet back towards earth.<br />

3. The specifications for Dominator are a 4.g launch and landing. You probably noticed the 4g<br />

reading but did not find 4g’s in your calculations, why? (Hint: average vs. constant<br />

accelerations)<br />

4. How do the average and maximum values compare? Did you observe linear or nonlinear<br />

accelerations? If they are linear with zero as one end point you can use the numeric<br />

average. Did that work here?<br />

28


Dominator Part II, The Drop Side: or Work/Energy on the bounce……<br />

By using the inclinometer and standing at some convenient distance from the base of<br />

Dominator, find the angle of incline for the maximum height and height after the first bounce.<br />

Angle at maximum height ____________________________(note this is 52 meters of altitude)<br />

Angle where riders begin deceleration=____________________________<br />

Angle at max height after first bounce ___________________________<br />

By using trigonometry, calculate the height where deceleration begins and after first bounce.<br />

The Law of Sine’s works well or use a scaled drawing and find the distance from the ride to<br />

your measuring location.<br />

Height where deceleration begins=__________________<br />

Height after first bounce ______________________<br />

First measure a total time for the drop, then measure the time the riders are decelerating by<br />

watching their bodies. Arms and legs are a good cue to see when deceleration is occurring.<br />

T(drop)=_____________ seconds<br />

T(decel)= ____________seconds<br />

Calculate your energy at these two positions. The maximum Mechanical Energy is the sum of<br />

the potential energy at the top and kinetic energy gained during the launch. The ride applies<br />

g/2 acceleration for approximately 10 meters. The remainder is covered in the PE calculation.<br />

ME(max) = PE + F * d = mgh + mg/2*10m =<br />

___________________(units also)<br />

PE (first bounce) = m g hbounce=____________________________________(units also)<br />

29


1. How much energy was lost from maximum height to first bounce height?<br />

2. What is the efficiency of the pneumatic spring used to bounce you? (remember it<br />

should not be very elastic, they want you to stop eventually)<br />

3. Did you notice your fall was not “freefall” soon after launch? The pneumatic system<br />

begins your deceleration soon after launch. If it were not for that, what would your final<br />

speed be before the 10-meter main deceleration? Use KE=PE + Work to find your<br />

velocity.<br />

30


4. Compare this velocity with an approximation based on landing time and average<br />

deceleration of 2g’s. How do they compare?<br />

5. Since we know the distance the riders came to rest in, using the fact that change in<br />

energy is due to work done we can find the average force on you. Find F given<br />

F=Energy / distance (work/energy theorem).<br />

6. Compare this to the force found by change in momentum divided by time. (application<br />

of impulse/momentum calculations)<br />

7. In all cases above, we have used average values. Calculus students should use the linear<br />

change in acceleration and reanalyze questions 5 and 6 using the appropriate F/t and<br />

F/d graphs in the area below. This question is meant to be open ended. It is safe to<br />

assume the force varies linearly with distance increasing from 0 to the 4g force. Be<br />

careful when looking at the time values due to the distance/velocity relationship.<br />

31


The Sea Dragon<br />

(Part 1)<br />

The following two activities involve the use of the<br />

conservation of mechanical energy and Newton's Second Law to<br />

determine the maximum speed of the Sea Dragon. It is<br />

recommended that the student first observe the motion of the ride to<br />

determine when and where the ride undergoes the motion of a<br />

physical pendulum. The portion of the ride studied should be while<br />

the boat is traveling freely.<br />

Activity I - Maximum Speed Using Energy<br />

Objective: To determine the maximum speed of the Sea Dragon using the principle of<br />

conservation of mechanical energy.<br />

Procedure:<br />

1. Use the inclinometer to measure the maximum angle, , that the ride makes with<br />

the vertical.<br />

Maximum angle, _________________<br />

32


The Sea Dragon<br />

(Part 1)<br />

2. The length of the swing arm, L is 10.7 m. (See diagram above.) Knowing this and<br />

that the maximum angle determines the maximum height, h, use the following<br />

guide to find h.<br />

h = 10.7(l - cos) meters<br />

Maximum height, h_________________<br />

3. Assuming that mechanical energy is conserved, the potential energy at the<br />

maximum height is equal to the kinetic energy, KE, at the lowest point. The<br />

lowest point is where the boat is traveling freely with maximum speed, v.<br />

PE = KE<br />

mgh = 1/2(m)v 2<br />

Solve mgh = ½ (m)v 2 for v and then calculate the maximum speed, v.<br />

33


The Sea Dragon<br />

Maximum speed, v_________________<br />

(Part 1)<br />

Activity 2 – Maximum Speed Using Newton’s Second Law<br />

Objective: To determine the maximum speed of the Sea Dragon using Newton's Second<br />

Law and to compare this value to the speed found in Activity 1.<br />

1. Ride the Sea Dragon. Using a hand held vertical accelerometer measure the<br />

"g's" at the lowest point of the ride's swing. Remember that 1 g means you feel<br />

the seat exerting a force, FN, on you that is equal to your normal weight, making<br />

you feel you normal. Two "g's" mean that you feel like you weigh is twice your<br />

normal weight in that the seat exerts a force, FN, on you equal to twice your<br />

weight.<br />

Number of g’s at the lowest point: _________________<br />

2. Since the motion of the ride near the bottom of the swing is approximately<br />

uniform circular motion, Newton’s Second Law predicts that<br />

FN -Fg = (mv 2 )/r<br />

where,<br />

FN is your support force (the force that the seat exerts on you)<br />

Fg is your weight<br />

m is your mass<br />

v is your speed and is a maximum value<br />

r is the radius of curvature (10.7 m)<br />

Solve this equation for maximum speed, v.<br />

What is the maximum speed equation, solved for v =_________________<br />

3. Determine your support force by multiplying the number of “g’s” by your<br />

weight.<br />

34


The Sea Dragon<br />

What is the support force, FN_________________<br />

(Part 1)<br />

4. Determine your mass using Newton’s Second Law.<br />

m= Fg/g<br />

Where g is the acceleration due to gravity<br />

What is your mass, m_________________<br />

5. Calculate the maximum speed, v, using the equation in #2 of this Activity.<br />

What is your maximum speed, v_________________<br />

6. Compare the two speeds using a percentage difference. If the speeds do not<br />

agree, discuss possible sources of error.<br />

What is the comparison of two speeds_________________<br />

35


The Sea Dragon<br />

(Part 2)<br />

The following activity involves the use of oscillatory motion concepts. It is<br />

recommended that the student first observe the motion of the ride to determine when and<br />

where the ride undergoes the motion of a physical pendulum. The portion of the ride<br />

studied should be while the boat is traveling freely.<br />

Objective: To determine the period of oscillation of the Sea Dragon in two different<br />

ways.<br />

Procedure:<br />

1. Using a stopwatch, measure the period of oscillation of the Sea Dragon.<br />

1. period of oscillation, T (first way)_________________<br />

2. Assume that the ride behaves like a simple pendulum and calculate the period using<br />

the following equation:<br />

T =2(L/g) 1/2<br />

where,<br />

T is the period of oscillation<br />

L is the length of the pendulum (10.7 m)<br />

g is the acceleration due to gravity<br />

2. period of oscillation, T (second way)_________________<br />

3. Compare the two periods using percentage difference. Is the Sea Dragon a simple<br />

pendulum?<br />

36


White Water Landing<br />

Observations:<br />

White Water Landing will give you an opportunity to use<br />

the concepts of momentum and impulse to determine the forces<br />

acting on you during the “splashdown.”<br />

1a. After observing a number of boats “splashing down,” does<br />

the size of the splash vary or is it fairly constant?<br />

_____________________________<br />

1b. If it varies, what observable factors seem to influence the size of the splash?<br />

2a. Is there any time during the ride that riders appear to lunge forward?<br />

2b. If yes, where and why does this occur?<br />

Activity 1<br />

Determining the magnitude of the velocity of the boat before<br />

and after “splashdown"<br />

Potential Energy PE = mgh mass (x) gravitational field (x) height<br />

(Top of the incline)<br />

Kinetic Energy KE = 1/2 mv 2 1/2 mass (x) velocity squared<br />

(Bottom of the incline)<br />

gravitational field g = 9.8 m/s/s at <strong>Dorney</strong> <strong>Park</strong><br />

height of incline 25 meters<br />

Potential Energy Joules (J)<br />

Length of Boat 5.2 m<br />

Part (a) Velocity immediately before splashdown<br />

37


White Water Landing<br />

To find the approximate velocity of the boat immediately before splashdown, we<br />

can make the assumption that the Potential Energy of the boat at the top of the incline is<br />

completely converted to Kinetic Energy at the bottom.<br />

Find the Potential Energy of a passenger at the top of the incline:<br />

PE=___________<br />

Lets assume that all of the Potential Energy becomes Kinetic Energy at the bottom of<br />

the incline. Use the information already obtained to find the velocity at the bottom of<br />

the incline.<br />

Part (a): Before splashdown<br />

your mass<br />

(kg) = _______________<br />

Hint: To find your mass in kg, you may find it useful to know that the<br />

weight of a 1 kg mass on earth is approximately 2.2 pounds.<br />

height of incline<br />

gravitational field<br />

Potential Energy at top of hill<br />

Kinetic Energy at bottom of hill<br />

25 meters<br />

9.8 m/s/s<br />

(J) =_______________<br />

(J) =_______________<br />

Velocity at bottom of the incline (m/s) = _______________<br />

Part (b): After splashdown<br />

Measure the time for the complete boat to pass under the bridge (after it has completed its<br />

“splashdown”). Observe at least three boats and find the average time for a boat to pass<br />

under the bridge. Use the information concerning the length of a boat to find the average<br />

final velocity of the boat.<br />

Data Chart for Finding Velocity of the Boat Before and After “Splashdown”<br />

Time to pass<br />

under the<br />

bridge<br />

Trial 1 Time (s) Trial 2 Time (s) Trial 3 Time (s ) Average Time (s)<br />

Velocity after<br />

splashdown (m/s)<br />

38


White Water Landing<br />

Activity 2<br />

Determining momentum change and impulse acting during the “splashdown”<br />

Momentum is defined as the mass of an object times its velocity.<br />

Physicists represent the quantity of momentum with the letter p.<br />

momentum = mass x velocity<br />

or<br />

p = mv<br />

Use your own mass to determine the momentum of a passenger riding in a boat<br />

both before and after splashdown. As a result of the boat splashing down, the<br />

momentum of each passenger changes. Find the change in momentum of the abovementioned<br />

passenger.<br />

momentum change = momentum after splashdown - momentum before splashdown<br />

or<br />

p = pafter - pbefore<br />

(the symbol delta means change)<br />

Data Chart for Finding Momentum Changes<br />

pbefore<br />

(kg m/s)<br />

pafter<br />

(kg m/s)<br />

p<br />

(kg m/s)<br />

Momentum of an object is changed by the application of an impulse.<br />

Impulse is defined as the product of an applied force and the time that the force acts:<br />

Impulse = Force x Time for force to act<br />

or<br />

J = F t<br />

The impulse applied to the passenger is equal to the momentum change for the<br />

passenger.<br />

J = p<br />

39


White Water Landing<br />

The time that the force acts to change the momentum is approximately the same<br />

as the time that the “splash” lasts, since the splash is a result of the water applying an<br />

impulse to the boat and the boat applying an impulse on the water.<br />

Observe at least three “splashdowns” and time how long each splash lasts to find<br />

an average splash time. From this information, determine the size of the force required<br />

to change the momentum of a passenger with your mass.<br />

If mass is in kg and acceleration is in m/s/s, then the unit for force is a newton<br />

(symbol N).<br />

Data Chart for Finding Forces Acting<br />

Trial 1<br />

Splash time<br />

(s)<br />

Trial 2<br />

Splash time<br />

(s)<br />

Trial 3<br />

Splash time<br />

(s)<br />

Average<br />

Splash time<br />

(s)<br />

p<br />

(kg m/s)<br />

<br />

Impulse<br />

(kg m/s)<br />

FA = Average Applied<br />

Force - FA(N)<br />

Activity 3<br />

Comparing Forces<br />

You can now determine how the force applied to the rider to slow down compares<br />

with other forces. A common force with which to compare is your weight. Determine<br />

how the force applied compares to your weight by using the following:<br />

Force Factor = Applied Force/Weight<br />

Data Chart<br />

If mass is in kg and acceleration is in m/s/s, then the unit for force is a newton (symbol N).<br />

FA (N)<br />

Applied Force from<br />

Activity 2<br />

Fw (N)<br />

Your Weight = mass *<br />

9.8 m/s/s<br />

Force Factor<br />

40


White Water Landing<br />

Questions for Analysis:<br />

1. Compare your force factor with other students’ of different mass. Explain your<br />

observations.<br />

2. Predict the size of the force acting on the entire loaded boat (the boat has a mass of<br />

approximately 1000 kg when empty). Estimate the total mass of riders and boat.<br />

41


The Scrambler<br />

Introduction:<br />

The Scrambler consists of two sets of arms, the upper<br />

sweep arms and the lower arms, that have different radii<br />

and revolve around different points of rotation to<br />

produce varying forces. You will be studying the paths of<br />

these arms and the cars attached to them, along with<br />

their properties, such as angular velocity, tangential<br />

velocity, and centripetal force.<br />

Apparatus:<br />

Stopwatch, calculator<br />

Part I:<br />

Procedure<br />

Stand at some point around The Scrambler so that you can see the entire ride.<br />

Watch the ride rotate several times.<br />

1. What direction do the sweep arms appear to be rotating? (clockwise or<br />

counter-clockwise)<br />

_____________________<br />

2. What direction do the lower arms appear to be rotating? (clockwise or<br />

counter-clockwise)<br />

_____________________<br />

Do you notice anything about the ride that seems to be cyclical? Try focusing on<br />

one particular car or one spot along the outside of the ride.<br />

You may notice that each sweep arm returns to the same point along the outside<br />

of the rides’ path every revolution, but each lower arm (and attached car) does<br />

not.<br />

Before the ride starts, find a car that is closest to the fence surrounding The<br />

Scrambler. It should be pointing almost directly at you. Remember this car, as<br />

you will be following its motion.<br />

Laboratory courtesy of Andrew Snyder, Materials Engineering, Rensselaer Polytechnic Institute Page 42


The Scrambler<br />

3. As the ride is rotating, what do you notice about the group of 4 cars to which<br />

the car you picked out belongs?<br />

4. How many revolutions does it take for that car to return to the same point<br />

that it started at?<br />

____________________<br />

5. What is the length of the sweep arms and what is the circumference of their<br />

path?<br />

Length: _________________<br />

Circumference: ____________________<br />

6. What is the length of the lower arms and what is the circumference of their<br />

path?<br />

Length: _________________<br />

Circumference: ____________________<br />

Part II:<br />

Now you will need your stopwatch and calculator. When the ride is up to full<br />

speed, record the time it takes for the ride to rotate 3 times. The easiest way to<br />

do this is record the time it takes for one of the sweep arms to pass you 3 times.<br />

Then divide by 3 to calculate the time of one revolution.<br />

Time of 3 revolutions: _______________________<br />

Period (time of 1 revolution): _______________________<br />

Now calculate the angular velocity, keeping in mind that each revolution is<br />

2*pi radians and your period has the units seconds/revolution.<br />

Angular velocity (in radians/second):<br />

________________________________<br />

Laboratory courtesy of Andrew Snyder, Materials Engineering, Rensselaer Polytechnic Institute Page 43


The Scrambler<br />

The tangential velocity is simply the speed that the object is travelling in its<br />

circular path. This can be obtained by multiplying the angular velocity by the<br />

radius of the path, or the length of the sweep arms.<br />

Tangential velocity (in meters/second):<br />

_______________________________<br />

The next part is a little trickier. Your task is to calculate the time it takes for the<br />

group of 4 cars to rotate one revolution. The easiest way is to orient yourself to<br />

the ride the same way you were before, lined up with the closest car to the<br />

outside, and to time 4 rotations of the upper arm, while counting how many<br />

times the group of 4 cars spins in a full circle. (Remember: the car completes<br />

one spin every time it is swung to the outside of the fence, at the point furthest<br />

away from the middle of the ride)<br />

Time of 4 revolutions: ______________________<br />

Number of spins in 4 revolutions: _______________________<br />

Period (time of 1 spin): _____________________<br />

You can now calculate the angular and tangential velocities for the lower<br />

arms attached to the cars using the same method you used for the sweep arms.<br />

Angular velocity (radians/second): _________________________<br />

Tangential velocity (meters/second): _________________________<br />

Part III:<br />

Now that you have calculated the velocities of both sets of arms it’s time to use<br />

them to reveal some interesting things about The Scrambler. Do the cars on The<br />

Scrambler have a higher speed when they are closer to the center of the ride or<br />

when they are closer to the outside of the ride? Hopefully, your answer was<br />

they travel faster when they are closer to the inside of the ride. Why is this? The<br />

speed of the cars is a product of the tangential velocity of both sets of arms.<br />

The sweep arms are moving clockwise, while the lower set of arms are moving in<br />

a counter-clockwise motion. This causes the tangential velocities of each set<br />

of arms to work together when the cars are closer to the center of the ride and<br />

offset each other when the cars are at their furthermost point from the center.<br />

Laboratory courtesy of Andrew Snyder, Materials Engineering, Rensselaer Polytechnic Institute Page 44


The Scrambler<br />

Given the information provided above you should now be able to calculate the<br />

maximum and minimum speeds of the cars when the ride is at full speed. An<br />

important thing to remember when doing these calculations is that while the<br />

angular velocity is always constant, the tangential velocity varies as a<br />

function of the radius, or the distance of the object from the point of rotation.<br />

Also, remember that when the tangential velocities are opposing each other<br />

you need to make one positive and one negative.<br />

Radius of the lower arm at the point of maximum speed:<br />

__________________<br />

Radius of the sweep arm at the point of maximum speed<br />

(distance of the car from the point of rotation of the sweep arm):<br />

_____________________<br />

Tangential velocity of the car due to the lower arm at the point of<br />

maximum speed:<br />

_______________________<br />

Tangential velocity of the car due to the sweep arm at the point<br />

of maximum speed:<br />

_______________________<br />

Maximum speed of the car: _______________________<br />

Radius of the lower arm at the point of minimum speed:<br />

__________________<br />

Radius of the sweep arm at the point of minimum speed<br />

(distance of the car from the point of rotation of the sweep arm):<br />

_____________________<br />

Laboratory courtesy of Andrew Snyder, Materials Engineering, Rensselaer Polytechnic Institute Page 45


The Scrambler<br />

Tangential velocity of the car due to the lower arm at the point of<br />

minimum speed: _______________________<br />

Tangential velocity of the car due to the sweep arm at the point<br />

of minimum speed: _______________________<br />

Minimum speed of the car: ___________________ (does this answer<br />

surprise you?)<br />

Part IV:<br />

The final part of this exercise is to calculate the centripetal force on the rider<br />

at the innermost and outermost points on the ride’s path. This must be done<br />

similarly to the way you calculated the tangential velocity of the car at both<br />

points, as centripetal force is also a radius dependant value. The centripetal<br />

force always points toward the center of rotation for each set of arms, so be sure<br />

to make one positive and one negative, if needed.<br />

The equation for centripetal force is Force = mass * radius * (angular<br />

velocity) 2 . You can use your own mass (in kg) in this calculation. (1 kg = 2.2<br />

lbs.)<br />

Centripetal force on the rider at the innermost part:<br />

_______________________<br />

Centripetal force on the rider at the outermost part:<br />

_______________________<br />

Length of Sweep Arm: 4.23 meters<br />

Length of Lower Arm: 3.65 meters<br />

Pivot arm from pivot to car: 1.82 meters<br />

Laboratory courtesy of Andrew Snyder, Materials Engineering, Rensselaer Polytechnic Institute Page 46


The Wave Swinger<br />

A SWINGING TIME<br />

Introduction:<br />

The Wave Swinger is a fairly simple ride, but it does<br />

have some interesting aspects. The rate of the rotation of<br />

the ride is constant and there are only two forces acting on<br />

the swing itself. This allows the easy analysis used in Part<br />

IV. However, because the ride tilts, the plane of swing is<br />

not horizontal. This adds some interesting possibilities to<br />

the motion of the swing and rider.<br />

Part I<br />

Theory<br />

Shown below is a crude picture of a rider on the swing seat. The swing seat and<br />

rider will be treated as one object.<br />

Since the forces F 1 and F 2 (actually there are four) are in the same direction, they can be<br />

considered as a single force F 1 and F 2 = F. This is shown below.<br />

Procedure:<br />

Place all answers where indicated within the procedures.<br />

1. Is the force of the chain F or mg? ________________________<br />

47


The Wave Swinger<br />

2. The force mg is the force due to what phenomena?<br />

____________________________________________________<br />

3. Draw the diagonal across the parallelogram.<br />

4. The diagonal of the parallelogram is the magnitude of what force?<br />

____________________________________________________<br />

____________________________________________________<br />

5. The direction of the force in number 4 is the same as the:<br />

speed or acceleration of the object?<br />

____________________________________________________<br />

6. If the speed is constant, which acceleration is equal to (0), the tangential<br />

acceleration or radial acceleration?<br />

______________________________________________________________<br />

7. Is v 2 /r the tangential or radial acceleration?<br />

Note: radial is another name for centripetal.<br />

______________________________________________________________<br />

8. Noting that the diagram in #3 shows the net force (thus acceleration) to be slightly<br />

up, would you conclude that the swing is at a low or high spot in its rotational path?<br />

48


The Wave Swinger<br />

Part II<br />

Observations relating to the theory<br />

Procedure:<br />

Make the following observations of the ride.<br />

1. Using the outside swings only, does the weight on the swing effect the angle of the<br />

chains?<br />

____________________________________________________<br />

<br />

Note: comparing an empty swing to a loaded one can do this.<br />

2. Do the riders on the inside swings travel at a faster or slower speed than those riding<br />

on the outside swings?<br />

____________________________________________________<br />

3. Use the inclinometer (as shown in the diagram below) to measure the angle that the<br />

chains make with the vertical for when the swings are at their highest point and<br />

lowest point. Within experimental error, are they the same or different?<br />

____________________________________________________<br />

4. Which swings have the greater angle from the vertical? The outside swings or the<br />

inside swings?<br />

____________________________________________________<br />

49


The Wave Swinger<br />

Part III<br />

Observations to be made on the ride<br />

1. Watch the chain as the ride begins. Which way does it move relative to you?<br />

____________________________________________________<br />

2. As you ride, how does the force of the seat on your “bottom” feel at a low point as<br />

opposed to that at the high point in your rotational path?<br />

Note: This force variation is indicative of the force variation in the chain.<br />

____________________________________________________<br />

Objective:<br />

Part IV<br />

Numerical Analysis<br />

To determine whether the radial (centripetal) acceleration is equal to the acceleration<br />

value of g (tan ) where is the angle that the chains make with the vertical.<br />

Procedure:<br />

1. Use the inclinometer to measure the angle that the outer swings make<br />

with the vertical as shown in the figure of Part II, Procedure step 3. If<br />

you feel there is significant difference between the angle when the swings<br />

are at a low point and high point, record both angles.<br />

Angle Value (low point) ________________________________________________<br />

Angle Value (high point)________________________________________________<br />

2. Time the ride for five complete revolutions. ________________________<br />

*The radius used is given as 9.0 meters.<br />

50


The Wave Swinger<br />

Analysis:<br />

1. Calculate the predicted acceleration using g(tan ), where g= 9.8 m/s 2 . If<br />

you used two different angles do this, perform calculation twice.<br />

____________________________________________________<br />

2. Find the period of the swing. (This is the time for one revolution.)<br />

____________________________________________________<br />

3. Calculate the acceleration using a = 4 2 r/T 2 .<br />

____________________________________________________<br />

4. Compare the accelerations in Parts 1 and 3 using percent difference.<br />

____________________________________________________<br />

5. Bonus: Based on the force diagram and a vertical component of the chain<br />

force equal to mg, show how Newton's Second Law produces an<br />

acceleration of g(tan).<br />

51


The Physics of<br />

Since the Gravity Rides of the 1500’s, the<br />

concept of the roller coaster has been a<br />

thrilling challenge for both rider and engineer.<br />

In this lab, you will have the chance to test the design of Steel Force, the “longest,<br />

tallest, fastest coaster in the East.” This laboratory is divided into 3 sections. Each<br />

section is a necessary step to evaluate the next section, so work in order and go as far as<br />

your instructor requires. The sections will help you examine kinematics, work/energy<br />

theorem, and curvilinear motion. The diagram below shows the parts of the ride we<br />

will analyze.<br />

Data Point A:<br />

is anywhere about half way up the first hill. At this point, the<br />

chain drive system is pulling the train uphill at a constant velocity.<br />

Data Point B: is at the bottom of the first hill. At this point, there is a tunnel 34<br />

meters long. You will use the length of the tunnel to find the speed<br />

at this point on the ride.<br />

Data Point C:<br />

Data Point D:<br />

Data Point E:<br />

is at the top of the second hill, 49.1 meters above the ground. You<br />

will use the length of the train to find its speed here.<br />

is the spiral curve at the far end of the coaster. You will measure<br />

the time to go around the curve for one full revolution. The radius<br />

of this turn is 31 m.<br />

is the return camelback’s first “hump.” You will use the train<br />

length to find its speed at this point.<br />

All data can be logged on the Steel Force Data Sheet, which follows this lab. The data<br />

will help you complete the computations for all of the following sections.<br />

52


Steel Force<br />

Section #1<br />

Koaster Kinematics......<br />

One of the primary measurements we must take in physics is the motion value called<br />

speed. In this section, we will compute the speed and acceleration values at the five<br />

points of interest on Steel Force.<br />

In general, we will use:<br />

v =d /t and a = v /t.<br />

Speed at points A, C, and E:<br />

At these points you will compute speed by using train length divided by time<br />

taken to pass a point. The train is 19.6 meters long. Check your Steel Force Data<br />

Sheet for the time to pass a point on the track at each of these locations. Use the<br />

measured times and complete the calculations in the chart on the next page for<br />

each of the points A, C and E.<br />

Speed at point B:<br />

This is the tough one! The tunnel is 34 meters long. If you measure the time<br />

through the tunnel, it will be short and you can compute the speed by the basic<br />

equation in chart line #4.<br />

Can you think of a way of measuring this more accurately? If you can, take the<br />

measurement your way and the way described above, then compare. If not, see if<br />

you can find another group who has done this.<br />

Hint: the train is 19.6 meters long and its length will increase the time of passing a<br />

point.<br />

Speed at curve D:<br />

Your measure of the time around the curve, along with the distance traveled, will<br />

give you this solution in line #5.<br />

Acceleration on first hill:<br />

Now apply your acceleration equation to solve for the average acceleration on the<br />

first hill. This is done in line #6. You will need the velocity at the top and bottom<br />

of the hill (Data points A and B) and also the time down the hill. Measure the<br />

time from when the center of the train passes the top of the hill to when that point<br />

enters the tunnel.<br />

53


Steel Force<br />

Deceleration on second hill:<br />

Using the same type of calculation, find the deceleration rate when going up to<br />

point B in line #7.<br />

Line 1<br />

Line 2<br />

Line 3<br />

Line 4<br />

Line 5<br />

Line 6<br />

Line 7<br />

VA=19.6m/____________ seconds = ______________<br />

don't forget units<br />

VC=19.6m/____________ seconds = ______________<br />

units<br />

VE=19.6m/____________ seconds = ______________<br />

units<br />

VB=34 m/____________ seconds = ______________<br />

units<br />

VD=*62 m/_________ seconds = ______________<br />

units<br />

Ahill=V/t =(________-_________)/____________ = ______________<br />

units<br />

Ahill=V/t =(________-_________)/____________ = ______________<br />

units<br />

Section #2<br />

Using the Work/Energy Theorem......<br />

Once you have been lifted to the top of the first hill, your trip is entirely<br />

controlled by a simple concept in physics, work/energy. The motor drive system simply<br />

is designed to propel you to the top of the first hill. This motor/chain drive acts on you<br />

and the train but, for this example, we will only work with you (all other parts like the<br />

train and passengers are proportionately larger). We will work on the assumption that<br />

friction is negligible to make our calculations easier.<br />

54


Steel Force<br />

Up the first hill: As you are pulled up the hill, the motor system must apply a<br />

force parallel to the hill in order to move you along. This hill is at an angle of 25<br />

degrees.<br />

8. Find the force on you as you go up the hill:<br />

F parallel =__________________<br />

Note: Recall the equation F par = mg sin<br />

<br />

This force will be applied up the entire length of the hill, 144 meters.<br />

9. What work is done on you during this part of the trip?<br />

Work = ___________________<br />

Before going further, how much power is required to pull you up, if you reach the top in<br />

the amount of time that you found?<br />

Find this in both Watts and Horsepower.<br />

P = #9_______/_______ (time) = _____________watts = _____________hp<br />

(10)<br />

Now, back to Work... The work done on you in a frictionless environment would<br />

remain as part of the total mechanical energy.<br />

11. At the top of the hill, what two types of energy do you have?<br />

12. List them and compute their values for you below.<br />

Use your mass for this analysis:<br />

(11) E (total mechanical energy) = _______________+________________<br />

name of one<br />

name of the other<br />

(12) E (total mechanical energy) = _____________+____________ =<br />

compute P<br />

compute K<br />

Since this value will remain nearly constant between the first and second hills, find the<br />

values for the stored part of the energy at points B and C. Note the first hill (at B) is<br />

below the starting level by 1.5 meters.<br />

(13) P at B = _____________<br />

(14) P at C = _____________<br />

55


Steel Force<br />

The work done to get you to the top of the 61 meter hill can be found the same way as finding the<br />

stored energy.<br />

15. Using this type of calculation, what is the stored energy at the top of the hill?<br />

P at Top = _______________<br />

Does this compare favorably to your calculation from calculation #9? Why?<br />

_____________________________________________________________<br />

_____________________________________________________________<br />

_____________________________________________________________<br />

If we assume E initial =E final , we can use the equation:<br />

_______________ (value from 12) = P + K.<br />

With this we can solve for velocity at two points of interest, points B and C.<br />

E (12) = P + K therefore K = E (12) - P<br />

Find the values for the motion energy at B and C; then compute the velocity from the equation K<br />

=1/2 m v 2 .<br />

K B = _______________ therefore V B = _________________<br />

K C = _______________ therefore V C = _________________<br />

We have measured the velocity at points B and C. Using Work/Energy we have<br />

predicted it. Compare the two values. How do they compare? What sources of error exist and<br />

how bad were they? In the blocks below, assuming the actual measures from Section #1 to be<br />

accurate, compute experimental error and explain.<br />

Data Analysis at Point B<br />

Data Analysis at Point C<br />

56


Steel Force<br />

Section #3<br />

Curvilinear Motion and Vectors<br />

reaction forces<br />

The basic motion we experience on roller coasters was<br />

explained in the sixteenth century. We will look at these<br />

principles using the physics and trigonometry studied in class.<br />

When you are traveling in the train, your body is<br />

moving in a straight line until the track or gravity changes<br />

your motion. We will start by looking at changes in the<br />

horizontal motion that your train travels.<br />

Mg<br />

F c<br />

When you travel through the far point spiral, you are traveling at a speed calculated in<br />

equation. You have the radius and speed, so find the centripetal acceleration.<br />

a centripetal = V 2 /R = _______ 2 /31 meters = _________________<br />

The average angle of the track at this spiral is 44 o . Compare this to a vector<br />

diagram of the track’s gravitational force verses its centripetal force. Fill in the values<br />

and draw scaled reaction forces with resultant on the drawing above. What do you<br />

notice? Discuss below: (include not just values, but what you felt, which way the forces<br />

acted on you, etc.)<br />

57


Steel Force<br />

Points B, C and E are other interesting<br />

positions. In these areas, you have a combination of<br />

forces acting on you in the vertical directions. If we<br />

assume a person to be ideally viewed as shown, create<br />

a free body diagram (FBD) including the seat and<br />

gravitational forces on the rider. Use the dot to the<br />

right for your FBD.<br />

gravity<br />

seat force<br />

At point B, we will define the upward force of the seat to be N for normal force. The<br />

centripetal force is also upward and gravity is downward. From this, we can predict the<br />

seat force on you by applying Newton’s Second Law as follows:<br />

F = m a<br />

The values, that we can see from the FBD, expand to the following:<br />

N - m g = m v 2 /r, or N = m(g+v 2 /r)<br />

16. Since these values are all known, we can easily find the force on your body. The<br />

radius of the tunnel curve is 34m. Using your value for speed from (4) and your<br />

mass, find the seat force N.<br />

N = ___________________<br />

17. Divide this (16) by your weight and compare to your accelerometer reading.<br />

N/mg =_____________ g’s compared to ___________________ g’s<br />

58


Data Point A, You are looking for the<br />

velocity of the train going up the hill.<br />

Find the time for the train to pass a<br />

point on the hill.<br />

t =________________<br />

Data Taking Sheet for<br />

Side 1, Kinematics<br />

Data Point C, The velocity at the<br />

top of the second hill is again found<br />

using train length and<br />

Time, t, =_________________<br />

Data Point B, Finding the velocity at the<br />

bottom of the big hill. Use the time it takes<br />

the train to go through the tunnel. Be<br />

careful, it will be a very short interval......<br />

t =____________________<br />

Data Point E, The top of the first<br />

Camelback Hump will be used as<br />

a reference. Measure the time it<br />

takes the train to pass the very<br />

top point.<br />

t =_________________<br />

59<br />

Data Point D, To find the speed<br />

through the curve, use the<br />

circumference and time to pass a<br />

vertical point through one<br />

revolution.<br />

t =_______________


Data Taking Sheet for<br />

Side 2, Curvilinear Motion and Vectors<br />

Data Point A, As you go up the hill,<br />

which way do you feel a force?<br />

Using your accelerometer, find the<br />

acceleration you are experiencing.<br />

a=_______________<br />

Data Point A to B, as you accelerate down<br />

the hill, you should see your accelerometer<br />

reading change. Find the acceleration<br />

going down the hill and at the bottom.<br />

a down =__________ a bottom =__________<br />

Data Point E, What is the<br />

acceleration at the peak of this<br />

hump? Take a reading and listen<br />

to the train on the track. What do<br />

you notice?<br />

a=________________<br />

60<br />

Data Point D, We will need<br />

acceleration through this curve.<br />

Use your accelerometer to<br />

measure this value.<br />

a=________________


Energy Curves for Steel Force<br />

Objective: To investigate a rider’s energy curves for a portion of the Steel Force ride<br />

Equipment: stopwatch, scaled photo of Steel Force’s second hill (see Diagram 1 in data section),<br />

small ruler<br />

Note: In this investigation the x-axis runs along the track.<br />

Procedure:<br />

1. Determine the speed of the coaster at position A (0 meter). To do this, time how long it<br />

takes the 19.6 meter long train to pass position A and record. (See Diagram 1 in data<br />

section).<br />

2. Repeat step # 1 for each of the remaining positions (B through L).<br />

3. Record your weight in pounds.<br />

4. Using Newton’s Second Law and the fact that 1 pound equals 4.448 Newtons, calculate<br />

the rider’s mass in kilograms and record. Show your work in the analysis section.<br />

5. Determine the rider’s kinetic energy at each position and record.<br />

6. Using Diagram 1 with its provided scale (the 20 m width), determine the distance each<br />

position is from position A (0 meters) and record. Note: This distance is equal to the<br />

magnitude of the position, x.<br />

7. Using Diagram 1 with its provided scale (the 20 m width), determine the height each<br />

position is from the ground and record.<br />

8. Determine the potential energy of the rider at each position and record. Show your work<br />

in the analysis section.<br />

Special thanks to Jeff Wetherhold 61


Energy Curves for Steel Force<br />

Data:<br />

A, 0 m<br />

B<br />

C<br />

D<br />

E<br />

F<br />

G<br />

H<br />

height of hill = 46<br />

m<br />

I<br />

J<br />

K<br />

L<br />

20 m<br />

Diagram 1<br />

Length of train = 19.6 meters<br />

Rider’s weight = _____ pounds<br />

Rider’s mass = ______ kilograms<br />

Special thanks to Jeff Wetherhold 62


Energy Curves for Steel Force<br />

Position<br />

mark<br />

Position,x<br />

(m)<br />

A 0<br />

Position,y<br />

(m)<br />

Time to<br />

pass<br />

position<br />

mark<br />

Speed at<br />

position<br />

mark<br />

(m/s)<br />

Kinetic<br />

energy at<br />

position<br />

mark, K<br />

(J)<br />

Potential<br />

energy at<br />

position<br />

mark, U<br />

(J)<br />

Total<br />

energy at<br />

position<br />

mark, E<br />

(J)<br />

B<br />

C<br />

D<br />

E<br />

F<br />

G<br />

H<br />

I<br />

J<br />

K<br />

L<br />

Special thanks to Jeff Wetherhold 63


Energy Curves for Steel Force<br />

Analysis:<br />

1. Show work for finding the rider’s mass.<br />

2. Show work for finding the rider’s kinetic energy.<br />

3. Show work for finding the rider’s potential energy.<br />

4. Using the provided graph paper, graph the kinetic energy, the potential energy, and the<br />

total energy as a function of the position, x. Plot the energies on the same set of axes.<br />

5. Based on analysis # 4 results, construct the corresponding net force vs. position graph<br />

(use the same piece of graph paper that you used for analysis # 4).<br />

6. According to the net force vs. position graph, what is the net force on the rider at the<br />

top of the hill? Does this make sense to you? Explain.<br />

7. Is the mechanical energy of the rider conserved? If not, what happens to the lost<br />

mechanical energy?<br />

Special thanks to Jeff Wetherhold 64


Centripetal Force and Steel Force<br />

Objective: To determine the centripetal force on a person riding Steel Force<br />

Equipment: stopwatch, scaled photo of Steel Force’s second hill (see Diagram 1 in data section),<br />

small ruler<br />

Procedure:<br />

1. Have someone ride the Steel Force and measure, with the vertical accelerometer,<br />

the “g-force” at the top of the second hill (see Diagram 1) and record.<br />

2. Time how long it takes the 19.6 meter long train to pass the top and record.<br />

3. Record the rider’s weight in pounds.<br />

4. Using Diagram 1 and its scale, determine the radius of the curvature of the hill at the top<br />

and record.<br />

Data:<br />

TOP<br />

20 m<br />

Diagram 1<br />

Special thanks to Jeff Wetherhold 65


Centripetal Force and Steel Force<br />

g-force at top of hill = _______ g<br />

length of train = 19.6 meters<br />

time for train to pass top = ______ seconds<br />

rider’s weight, W = ______ pounds<br />

radius of curvature of the second hill at the top, r = ______ meters<br />

Analysis:<br />

1. Draw a force diagram for the rider at the top of the hill. The forces involved include the<br />

normal force, F N and weight, W.<br />

2. Knowing that 1 pound equals 4.448 Newtons, determine the rider’s weight, W in Newtons.<br />

3. Knowing the g-force on the rider, determine the normal force on the rider at the top. For<br />

example, if the rider measured 2 g’s, then the normal force on the rider would be equal to<br />

two times the rider’s weight.<br />

4. Using Newton’s Second Law and the fact that 1 pound equals 4.448 Newtons, calculate<br />

the rider’s mass, m in kilograms.<br />

5. The centripetal force on the rider is equal to the net center directed force, Σ F on the<br />

rider. Use this fact to determine the centripetal force, F c on the rider at the top.<br />

6. Knowing the length of the train and the time for the train to pass the top, determine the<br />

speed, v of the rider at the top of the hill.<br />

7. Knowing that acceleration of the rider at the top is given by the equation ac =<br />

v 2 ,<br />

r<br />

determine the rider’s acceleration.<br />

8. From Newton’s Second Law, the centripetal force on the rider is also equal to the rider’s<br />

mass times the rider’s acceleration or F <br />

= māc . Use this fact to determine the<br />

c<br />

centripetal force on the rider at the top.<br />

9. Using a % difference, compare the centripetal forces you found in analysis # 5 and # 8.<br />

Special thanks to Jeff Wetherhold 66


The Talon will allow the opportunity to study the forces that act as your body goes through a variety of<br />

loops and curves. Before riding, spend some time looking at the ride. If possible watch a number of trains<br />

going through the complete circuit.<br />

1. Describe what your body would expect to feel at the following points on the ride:<br />

(See the accompanying diagram to identify these points)<br />

o Bottom of the first hill:<br />

o Top of the vertical loop (when you are upside down):<br />

o As you pass through the top of the Zero “g” Roll<br />

(the title of this element may be helpful!):<br />

o The middle of the horizontal Spiral:<br />

Mass in kg =<br />

Formulas required for these activities:<br />

Weight in pounds/2.2<br />

Magnitude of velocity = Distance traveled/time interval or v = d/t<br />

Centripetal acceleration = Velocity squared divided by radius or a C =v 2 /r<br />

Centripetal Force = Mass times centripetal acceleration or F = ma c<br />

Force due to gravity<br />

(weight) =<br />

Mass times gravitational acceleration or F g =mg (g = 9.8 m/s/s at<br />

<strong>Dorney</strong> <strong>Park</strong>)<br />

Force Factor = Seat Force/Force of Gravity or FF = F s /F g<br />

67


Most of the required measurements can be taken while observing the Talon from the area around the<br />

Antique Carousel near the Main Gate.<br />

Part 1 - Determining the magnitude of the velocity at key points on the ride.<br />

Observe some cars traveling through the ride. Find the magnitude of the velocity of the cars as they pass<br />

each of the following locations. To find the velocity, use the length of the train (12.2 meters) and measure the<br />

time it takes the complete train to pass a certain point. Be sure to collect data for at least three trials and average<br />

your results. Measure time in seconds (s) and calculate the velocity in meters per second (m/s)<br />

Bottom of the first hill:<br />

Length of Train = 12.2 m<br />

Time for train to pass the point = _______________<br />

Magnitude of the velocity of train = ____________________________<br />

Top of the vertical loop (when you are upside down)<br />

Length of Train =12.2 m<br />

Time for train to pass the point = _______________<br />

Magnitude of the velocity of train = ____________________________<br />

At the peak of the Zero “g” Roll<br />

Length of Train = 12.2 m<br />

Time for train to pass the point = _______________<br />

Magnitude of the velocity of train = ____________________________<br />

In the middle of the horizontal Spiral<br />

Length of Train = 12.2 m<br />

Time for train to pass the point = _______________<br />

Magnitude of the velocity of train = ____________________________<br />

68


Part 2 - Determining the accelerations and forces acting on a rider at key points:<br />

You will need to have your mass in kg determined: Your mass = ___________kg<br />

The accelerations and forces experienced moving through a curve or loop can be considered by using<br />

the principles of circular motion.<br />

Bottom of the first hill:<br />

Radius of curve= 25.0 m<br />

Centripetal Acceleration = ____________<br />

velocity (from part 1) = ______________<br />

Centripetal Force = _________________<br />

Top of the vertical loop (when you are upside down):<br />

Radius of curve= 6.0 m<br />

velocity (from part 1) = _____________<br />

Centripetal Acceleration = ____________<br />

At the peak of the Zero “g” Roll<br />

Radius of curve= 18. 0 m<br />

Centripetal Acceleration = ____________<br />

In the middle of the horizontal Spiral<br />

Radius of curve= 9.1 m<br />

Centripetal Acceleration = ____________<br />

Centripetal Force = ________________<br />

velocity (from part 1) = _____________<br />

Centripetal Force = ________________<br />

velocity (from part 1) = _____________<br />

Centripetal Force = ________________<br />

69


Part 3: Determining the force that a rider feels at key points and calculating expected “g” forces.<br />

In addition to moving along the curve, a force is also required to “hold you up”. This additional force<br />

would be an upward force equal in amount to your weight. The centripetal forces that you calculated in Part 2<br />

are simply a combination of the force that the seat exerts (Fs) and the force due to gravity (Fg). The force due<br />

to gravity is often referred to as your weight. Calculate your weight in Newtons.<br />

Force due to gravity (weight) = ____________________N<br />

Bottom of loop.<br />

Fc is up, so<br />

F c =F s -F g<br />

Seat Force F s = F c +F g<br />

Fs<br />

Top of loop.<br />

This situation works for top<br />

of vertical loop and top of<br />

Zero “g” roll<br />

Fc is down, so<br />

F c =F g +F s<br />

Seat Force F s = F C -F g<br />

Fs<br />

Fg<br />

Fg<br />

Your weight in newtons = __________________N<br />

Bottom of the first hill:<br />

Centripetal Force (from part 2)= ____________N<br />

Seat Force = ____________________N<br />

Top of the vertical loop (when you are upside down):<br />

Centripetal Force (from part 2)= ____________N<br />

Seat Force = ____________________N<br />

70


At the peak of the Zero “g” Roll<br />

Centripetal Force (from part 2)= ____________N<br />

Seat Force = ____________________N<br />

Analysis of the forces in the horizontal spiral requires knowledge of vector mathematics. This analysis may<br />

be optional.<br />

The forces in the horizontal spiral are a bit more complicated, the centripetal force is a combination of the force<br />

required to hold you up (opposite of force of gravity) and the seat force, both of which are vectors.<br />

Since these are vectors that are not parallel to one another you need to use vector addition techniques.<br />

Seat Force<br />

(Fs)<br />

Force holding you<br />

up = your weight<br />

(Fg)<br />

From the Pythagorean Theorem:<br />

Centripetal Force<br />

(Fc)<br />

Fs 2 = Fg 2 + Fc 2<br />

In the middle of the horizontal Spiral<br />

Centripetal Force (from part 2)= ____________N<br />

Seat Force = ____________________N<br />

Part 4: Calculated “g” Forces:<br />

Of interest to many roller coaster enthusiasts are the “g” forces experienced at various places on the ride.<br />

Use the calculations you have just completed to find the Force Factor (or “g” forces) that you can expect at<br />

the key points on the ride.<br />

Bottom of the first hill:<br />

Seat Force (from part 3)= ____________N Predicted Force Factor (“g” force) = ______________<br />

Top of the vertical loop (when you are upside down):<br />

Seat Force (from part 3)= ____________N Predicted Force Factor (“g” force) = ______________<br />

At the peak of the Zero “g” Roll<br />

Seat Force (from part 3)= ____________N Predicted Force Factor (“g” force) = ______________<br />

In the middle of the horizontal Spiral<br />

Seat Force (from part 3)= ____________N Predicted Force Factor (“g” force) = ______________<br />

71


Part 5: - Measuring “g’s”<br />

Someone in your group needs to ride the roller coaster. Using your vertical accelerometer (long tube)<br />

measure the g's at the points being studied. Remember 1 g means that you feel forces equal to your weight,<br />

2 g’s mean that you feel forces that are double your weight, etc. To measure g forces, hold the accelerometer<br />

parallel to your body (perpendicular to the lap bar). As you ride, try to remember the readings as you pass<br />

through each of the key points, do not attempt to write down the readings in the midst of the ride!!!<br />

Bottom of the first hill:<br />

Measured “g” Force = ______________<br />

Top of the vertical loop (when you are upside down):<br />

Measured “g” Force = ______________<br />

At the peak of the Zero “g” Roll<br />

Measured “g” Force = ______________<br />

In the middle of the horizontal Spiral<br />

Measured “g” Force = ______________<br />

72


Questions for Analysis:<br />

1. Which of the four points has the rider traveling at the greatest speed? Explain why this is the fastest of<br />

the four points. <strong>Dorney</strong> <strong>Park</strong> ads say that Talon reaches speeds of 58 mph, how do your results compare<br />

to this claim? (either convert your results to mph or convert 58 mph to m/s to do the comparison)<br />

2. Compare the calculated force factors at each point to the measured force factors. Why may there be<br />

some differences?<br />

3. Why do they refer to the third element studied as the Zero “g” Roll? Do your results seem to agree with<br />

this claim?<br />

4. Why is the radius of the vertical loop so much smaller at the top than at the bottom? How do you think<br />

the experience of Talon would be affected if the vertical loop had a large radius at the top (like it does at<br />

the bottom)?<br />

5. Describe what factors make Talon exciting and different from other coasters like Steel Force or<br />

Hercules? If you studied another coaster, compare the results and explain what makes the other coaster<br />

exciting and different from Talon.<br />

73


Inclined Spiral<br />

Immelman<br />

Zero “g” Roll<br />

Horizontal Spiral<br />

Vertical Loop<br />

Bottom of First Hill


Thunderhawk<br />

An Enlightening Lab<br />

Introduction:<br />

Thunderhawk is the original roller coaster for <strong>Dorney</strong> <strong>Park</strong>. Although it looks small compared to<br />

Steel Force it is an excellent ride in design and function. As with all wooden type coasters the vibrations<br />

are part of the experience. It is for this reason this lab has no measurements taken on the ride though it is<br />

highly recommended you ride it to experience the usual thrills and also the decrease in energy as you<br />

move from beginning to end.<br />

Purpose:<br />

To measure the lost mechanical energy from the top of the first hill to the small hump near the<br />

end of the ride.<br />

Theory:<br />

There are no blueprints of this 1923 ride so all measurements must be determined by you.<br />

Position yourself in the vicinity of the ride called, Possessed so that you have an unobstructed view of the<br />

first hill of the Thunderhawk. In line with the top of the hill and approximately twelve feet off the<br />

ground you will see a red spot. Notice that this spot is the same height as the small hump behind the hill.<br />

See figure one. This small hump is near the end of the ride. This height will be zero potential energy,<br />

thus when the coaster goes over the small hump it will have all kinetic energy and no potential energy.<br />

Note: potential energy is based on position relative to a zero reference level. Any height below<br />

the red spot would be a negative potential energy and the kinetic energy would be more than our value.<br />

Top of hill<br />

6 ft<br />

Top of hump<br />

Red dot<br />

Figure 1<br />

75


Thunderhawk<br />

An Enlightening Lab<br />

You will find the mechanical energy you have left at the top of the small hump as a percentage of<br />

the mechanical energy you have at the top of the first hill. Since energy is conserved this "lost"<br />

mechanical energy is actually converted to small molecular motions associated with thermal energy.<br />

This percentage is in a sense a measure of our coaster's efficiency.<br />

Equations:<br />

1. Top of the first hill:<br />

Total MechanicalEnergy PE KE mgh 1 mv 2<br />

2<br />

2. Top of the hump:<br />

Total MechanicalEnergy KE 1 2 mV 2<br />

3. Fraction of Mechanical Energy Remaining<br />

<br />

<br />

1<br />

2 mV2<br />

mgh 1 2 mv2<br />

1<br />

2 V 2<br />

gh 1 2 v2<br />

(mass cancels)<br />

V 2<br />

<br />

2 gh v 2 (multiplyby two)<br />

4. Percentage of Mechanical Energy Remaining<br />

<br />

<br />

<br />

<br />

<br />

<br />

V 2<br />

<br />

2gh v 2 100<br />

<br />

76


Thunderhawk<br />

An Enlightening Lab<br />

Procedure and Data:<br />

1. Using the red spot as h = 0 determine the height of the first hill given that the vertical boards are 6 feet<br />

long. Notice we will be using English units, so g = 32 ft/s 2 . Also the nearest whole foot will be uncertain<br />

so generally we will be working with two significant digits.<br />

Estimated height of hill as measured from the red spot<br />

h = _____ feet<br />

2. The trains are 40 ft long. Measure the time it takes the entire train to pass a vertical rail at the top of<br />

the hill.<br />

time = _________ seconds<br />

3. Now measure the time it takes an entire train to pass over the small hump behind the first hill. This is<br />

near the end of the ride. You can use the top of the hump as the reference point. You can move your<br />

position to line up a vertical board with this spot.<br />

time = _________ seconds<br />

Calculations:<br />

1. Calculate the speed v in ft/s as the train passes over the first hill.<br />

2, Calculate the speed V in ft/s as the train passes over the hump.<br />

3. Use equation 4 from the theory to calculate the percentage of the energy remaining near the end of the<br />

ride.<br />

77


Thunderhawk<br />

An Enlightening Lab<br />

Want an "A”? Answer the following:<br />

1. If the weight of the train is 4000 pounds find the potential energy at the top of the first hill. Note: the<br />

unit "pounds" is weight, therefore mg = 4000 pounds so just multiply by h.<br />

The unit will be ft-lb.<br />

2. Find the mechanical energy "LOST" during the ride.<br />

3. If this energy were heat what would be the temperature increase of a cup of water (0.52 lbm) if the<br />

specific heat of the water were 1 BTU / ( lbm o F). Assume no heat was used to heat the container. 1 BTU<br />

= 778 ft lb A BTU is a British Thermal Unit<br />

78


The Hydra<br />

Introduction: This experiment is written in three different parts. Lab 1 will be using the speed of the<br />

Hydra train at various places on the ride along with the radius of curvature of the track at those locations<br />

to calculate the force factor that the rider experiences. Lab 2 will also calculate force factor but this time<br />

the track is banked which makes the problem a little more challenging. Lab 3 will be calculating the total<br />

amount of energy at various places looking at the amount of energy lost throughout the ride.<br />

Preliminary Data:<br />

The information found in the Preliminary Data section will be used throughout the Hydra Labs.<br />

Equipment needed:<br />

Stopwatch<br />

Vertical accelerometer<br />

Special thanks to Brent Ohl 79


The Hydra<br />

C<br />

D<br />

A<br />

B<br />

G<br />

E<br />

F<br />

Measure the time it takes the train to pass the reference points shown below. Start the stopwatch when<br />

the front of the train reaches the reference point and stop the stopwatch when the back of the train reaches<br />

that point. The pictures will help you find the reference points. It is recommended that at least two<br />

people measure the time and take the average for more accurate results. Enter the values of time in Table<br />

#1.<br />

Point A:<br />

The bottom of the first hill. Look for the red dot on the middle of the track.<br />

Special thanks to Brent Ohl 80


The Hydra<br />

Point B:<br />

The top of the zero-g roll. Use the track junction as the reference.<br />

Point C:<br />

Point D:<br />

The bottom of the hill just after the zero-g roll. Look for the red dot.<br />

The middle of the cobra roll (a.k.a. Happy Face). Use the support post as the reference<br />

point.<br />

Point E:<br />

The top of the camel back just after the train passes the station. Use the support post as<br />

the reference point.<br />

Point F: The middle of the spiral near the end of the ride. Use the support post as the<br />

reference point.<br />

Point G:<br />

The end of the ride just before entering the breaking segment. Use the first vertical post<br />

on the handrail as the reference point.<br />

Now ride Hydra and measure the force factor at Points A-F using the vertical accelerometer holding it<br />

parallel to your upper body. Once again, it would be best if at least two people measure the force factor<br />

and compare them for more accurate results. Enter the values for the force factor in the table below.<br />

In the table below use the descriptors; lighter, heavier, or same to describe the sensation you experienced<br />

at the designated locations in reference to how you feel motionless, upright.<br />

Special thanks to Brent Ohl 81


The Hydra<br />

Knowing the that the length of the train is 12.298 meters long, ∆x, and<br />

train at the designated locations.<br />

x<br />

v , calculate the speed of the<br />

t<br />

Table #1<br />

Track<br />

Section<br />

A<br />

Time, ∆t<br />

(seconds)<br />

Train Speed, v<br />

(m/sec)<br />

Force<br />

factor<br />

Sensation<br />

(lighter, heavier,<br />

same)<br />

B<br />

C<br />

D<br />

E<br />

F<br />

G XXX XXX<br />

This information will be used throughout the three labs for Hydra.<br />

Your weight in lbs, Fw = ________________ x 4.45 N = __________________N<br />

lbs<br />

Your mass in kg, m =<br />

F w<br />

g<br />

______________________ kg<br />

Special thanks to Brent Ohl 82


The Hydra<br />

Lab 1—Force Factor Analysis<br />

Using the orientation represented in the picture for each location, draw the force diagram of the rider.<br />

Then use Newton’s laws to calculate the force of the seat and force factor experienced by the rider. The<br />

radii of curvatures are given for each part. The speed of the train was calculated in table #1.<br />

Part A<br />

Radius of the track, r = 26.25 m<br />

Calculate the seat force using:<br />

F<br />

seat<br />

F<br />

w<br />

mv<br />

<br />

r<br />

2<br />

F<br />

force factor <br />

F<br />

seat<br />

w<br />

___________<br />

Part B – top of zero-g roll<br />

Radius of the track, r = 16.0 m<br />

Calculate the seat force using:<br />

F<br />

w<br />

F<br />

seat<br />

mv<br />

<br />

r<br />

2<br />

Fseat<br />

force factor ___________<br />

Fw<br />

Part C – After zero-g Roll<br />

Radius of the track, r = 20.8 m<br />

Calculate the seat force using:<br />

F<br />

seat<br />

F<br />

w<br />

mv<br />

<br />

r<br />

2<br />

Special thanks to Brent Ohl 83


The Hydra<br />

F<br />

force factor <br />

F<br />

seat<br />

w<br />

___________<br />

Part D—Cobra Roll (a.k.a. Happy Face)<br />

Radius of the track, r = 15.5 m<br />

Calculate the seat force using:<br />

F<br />

seat<br />

F<br />

w<br />

mv<br />

<br />

r<br />

2<br />

F<br />

force factor <br />

F<br />

Part E—Camel Back<br />

Radius of the track, r = 16.0 m<br />

Calculate the seat force using:<br />

seat<br />

w<br />

F<br />

___________<br />

w<br />

F<br />

seat<br />

mv<br />

<br />

r<br />

2<br />

F<br />

force factor <br />

F<br />

seat<br />

w<br />

___________<br />

Special thanks to Brent Ohl 84


The Hydra<br />

Questions:<br />

1. How do the force factors you experienced while riding compare to the force factors you<br />

calculated using Newton’s laws? Why are the values not exactly the same?<br />

2. The force factors experienced from the Camel Back and the Zero-g Roll are the same, but<br />

the orientation of the rider is very different. Why is this the case?<br />

Lab 2: Force<br />

Factor on the<br />

Spiral—The<br />

Banked Curve of<br />

This activity is designed for the Honors/Advanced Placement Physics student.<br />

The radius of curvature of the spiral is 16.1 m.<br />

Using the diagram below, draw the force diagram of the rider while on the spiral (Point F) described in<br />

the preliminary data section. Assume there are no forces applied to the rider that are parallel to the seat.<br />

Special thanks to Brent Ohl 85


The Hydra<br />

Front view of the rider<br />

Using the force diagram along with force factor and speed of the train you found in the preliminary data<br />

section, generate the equation for the banking angle of the spiral.<br />

Calculate the banking angle of the spiral:<br />

Banking Angle, θ = _______________________<br />

According to your force diagram, generate another equation to calculate the banking angle of the spiral<br />

and solve for it.<br />

Banking Angle, θ = ____________________<br />

Special thanks to Brent Ohl 86


The Hydra<br />

Analysis:<br />

According to the force diagram, we made the assumption that there are no parallel forces applied<br />

to the rider by the seat. This means that the banking angle of the track is perfect. When dealing with<br />

roller coasters, this typically does not happen. This way the train “searches” for equilibrium, and the<br />

train will wobble from side to side while traveling around the curve similar to that of a passenger train.<br />

So, engineers correct this problem by not making the banking angle perfect. Does your data verify this?<br />

Explain.<br />

Special thanks to Brent Ohl 87


The Hydra<br />

Lab 3: Work/Energy<br />

considerations using<br />

Equipment needed:<br />

Stopwatch<br />

Inclinometer<br />

Power of the chain lift:<br />

Hold the inclinometer parallel to the lift hill and record the angle of the lift hill below:<br />

Angle of incline: _________________<br />

Calculate the force of the chain lift, F|| to get the 12,560 kg train to the top of the hill assuming the train<br />

moves up the hill at constant speed.<br />

F||<br />

θ<br />

mg<br />

θ<br />

mg sinθ<br />

F|| = mg sinθ = ___________________<br />

Measure the total time the front car of the train takes to make it up the lift hill.<br />

Time, t = ______________________<br />

Calculate the average speed v of the lift hill chain knowing the hill is 69.5 m long.<br />

d<br />

v = _________________<br />

t<br />

Calculate the amount of work done by the chain to lift the train up the hill.<br />

Special thanks to Brent Ohl 88


The Hydra<br />

W = F|| d = ______________________<br />

Calculate the power output of the chain lift motor in watts and horsepower knowing there is 746W/hp.<br />

P =<br />

W<br />

t<br />

_______________Watts = ___________________hp<br />

Compare the power found above to the power calculated by using the following equivalent equation:<br />

P = F|| v = ______________________<br />

Total Energy of the train at various locations along the track (NOTE: All track height measurements<br />

will be in reference to the bottom of the first hill)<br />

Keeping in mind that gravitational potential energy is represented by the following equation:<br />

and kinetic energy is given by the equation:<br />

PE = mgh<br />

You can now find the total energy at any given point on the track by<br />

1 KE mv<br />

2<br />

2<br />

Where mass m is the mass of the train.<br />

TE = PE + KE<br />

Calculate the energy at the top of the lift hill: The lift hill is 32.1m.<br />

PE = _________________________<br />

KE = __________________________<br />

TEinitial = ______________________________<br />

Calculate the energy at Point A: The height at A is 0 m above the bottom of the lift hill.<br />

PE = _________________________<br />

TEA = _________________________<br />

KE = __________________________<br />

TEinitial - TEA = ______________________<br />

Special thanks to Brent Ohl 89


The Hydra<br />

Calculate the energy at Point B: The height at B is 20.2 m above the bottom of the lift hill.<br />

PE = _________________________<br />

TEB = _________________________<br />

KE = __________________________<br />

TEinitial – TEB = ______________________<br />

Calculate the energy at Point C: The height at C is 5.5 m above the bottom of the lift hill.<br />

PE = _________________________<br />

TEC = _________________________<br />

KE = __________________________<br />

TEinitial – TEC = ______________________<br />

Calculate the energy at Point D: The height at D is 8.5 m above the bottom of the lift hill.<br />

PE = _________________________<br />

TED = _________________________<br />

KE = __________________________<br />

TEinitial – TED = ______________________<br />

Calculate the energy at Point E: The height at E is 10.1 m above the bottom of the lift hill.<br />

PE = _________________________<br />

TEE = _________________________<br />

KE = __________________________<br />

TEinitial – TEE = ______________________<br />

Calculate the energy at Point F: The height at F is 6.1 m above the bottom of the lift hill.<br />

PE = _________________________<br />

TEF = _________________________<br />

KE = __________________________<br />

TEinitial – TEF = ______________________<br />

Calculate the energy at Point G: The height at G is 7.3 m above the bottom of the lift hill.<br />

PE = _________________________<br />

TEG = _________________________<br />

KE = __________________________<br />

TEinitial – TEG = ____________________<br />

Special thanks to Brent Ohl 90


The Hydra<br />

The work energy theorem Wbrakes = KE can be used to calculate the average force needed to stop the<br />

train when it reaches the braking section of the ride.<br />

The kinetic energy of the train just before the brakes are applied is the KE at Point G.<br />

The kinetic energy of the train when the train stops is<br />

KEG = ________________________<br />

KEstop = _______________________<br />

Calculate the amount of work needed to stop the train:<br />

Wbrakes = _____________________<br />

Calculate the average force applied to the train by the brakes knowing W = Fd and the distance the brakes<br />

are applied to the train is 6.2 m.<br />

Fbrakes = _______________________<br />

Questions:<br />

1. Is the total energy the same at every point on the track you measured? Should it be the<br />

same—Explain.<br />

2. How much energy was lost on the ride? What is the cause of this loss of energy?<br />

3. It was mentioned previously that the brakes apply an average force to the train. Explain<br />

why it is an average force and not an instantaneous force.<br />

Special thanks to Brent Ohl 91


The Hydra<br />

4. You calculated the total amount of energy of the train at the top of the lift hill. Where did<br />

that energy come from?<br />

Critical Thinking Problem:<br />

Try to calculate the average frictional force applied to the train starting at the top of the lift<br />

hill to Point G given the length of the track being approximately 810 m.<br />

Lab 4: The JoJo<br />

Roll of. . .<br />

This is a short conceptual activity using the JoJo Roll of the Hydra. The JoJo roll is the first element<br />

when leaving the station. This element is quite unique to roller coasters.<br />

Part 1<br />

Go to the Cobra Roll side of the ride facing the "happy face" to get a front view of the train<br />

Special thanks to Brent Ohl 92


The Hydra<br />

passing through the JoJo Roll.<br />

Question:<br />

1. Estimate your force factor just before entering the roll. Explain your reasoning.<br />

2. Estimate your force factor when you are upside down in the roll. Explain your reasoning.<br />

Special thanks to Brent Ohl 93


The Hydra<br />

Part 2:<br />

While riding through the JoJo Roll, hold one vertical accelerometer upside down, hold one horizontally<br />

left, hold one horizontally right, and hold one right side up.<br />

Questions:<br />

1. What was the difference in force factor during the JoJo Roll? Explain your reasoning.<br />

2. Compare the JoJo roll to other roller coasters that go upside down with regards to the<br />

weightless feeling and the force factor.<br />

3. Since you are going upside down, can you do something to the ride to create a weightless<br />

feeling on the JoJo roll? Why/Why not.<br />

4. The JoJo is considered a heartline roll. By watching the train pass through the roll, explain<br />

the meaning of heartline roll.<br />

Special thanks to Brent Ohl 94


Interpreting Graphs<br />

Part I: - Directions: Using Graph 1 and 2 below answer the questions found below the graphs.<br />

Graph 1: Dominator: Shot Downward<br />

Questions:<br />

1. A. If you and a friend were watching and waiting in line to ride the Dominator,<br />

at what point of the drop would you tell him/her on the ride that they will<br />

experience a feeling of weightlessness?<br />

B. At what time interval does this occur at according to the graph?<br />

____________________________________<br />

2. If zero altitude is your starting position on the Dominator, according to the<br />

graph how high does the Dominator climb before dropping you?<br />

__________________________________<br />

3. The same friend you advised in question #1 is afraid that the Dominator is<br />

going to drop straight to the ground. According to graph 1, how much distance<br />

is between the ground and the lowest point on the first drop?<br />

__________________________________<br />

95


Interpreting Graphs<br />

4. From the graph of The Dominator, notice that the ride lasts longer than 120<br />

seconds. From your interpretation of the first 120 seconds of the ride, and after<br />

looking at the ride in the park, draw what you think the altitude and the x-<br />

acceleration due to gravity would look like if the graph actually took into<br />

account the ENTIRE ride.<br />

Hint: Take a stop watch and see how much longer the ride actually goes and<br />

how many more up and down motions the ride will experience after the 120<br />

seconds represented on the graph.<br />

Graph 2: Revolution<br />

5. According to graph #2 (Revolution), how many revolutions actually occurred in<br />

the 120 seconds?<br />

______________________________________________<br />

6. What is the correlation between the altitude and the G forces acting on the x-<br />

axis according to the data obtained from Revolution?<br />

_______________________________________________<br />

7. If you think of Revolution as a pendulum, at what point would you experience<br />

the greatest G forces? The highest peak or at the lowest point in the ride?<br />

___________________________________<br />

96


Interpreting Graphs<br />

Explain how you determined this by using specific references to the graph.<br />

______________________________________________________________________________<br />

______________________________________________________________________________<br />

______________________________________________________________________________<br />

______________________________________________________________________________<br />

________________________________________________<br />

8. After viewing the ride “Revolution” compare the graph to the actions of the<br />

actual ride. Notice again that the entire ride is not present on the graph. If<br />

“Revolution” runs an identical path each time it operates, do you think the g-<br />

force shown on the graph has reached its highest peak? If not, how many more<br />

peaks would there be before it reaches its highest peak?<br />

______________________________________________________________________________<br />

______________________________________________________________________________<br />

____________________________________________________________<br />

Part II<br />

Directions: For the following Graphs A – J, match the graph with the ride in<br />

<strong>Dorney</strong> <strong>Park</strong>. Answer the questions after all the graphs.<br />

Graph A<br />

97


Interpreting Graphs<br />

Graph B<br />

Graph C<br />

98


Interpreting Graphs<br />

Graph D<br />

Graph E<br />

99


Interpreting Graphs<br />

Graph F<br />

Graph G<br />

100


Interpreting Graphs<br />

Graph H<br />

Graph I<br />

Graph J<br />

101


Interpreting Graphs<br />

<strong>Dorney</strong> <strong>Park</strong> Ride<br />

Apollo 2000<br />

Wave Swinger<br />

Thunderhawk<br />

Steel Force<br />

The Hydra: Revenge<br />

Talon<br />

Enterprise<br />

Music Express<br />

Dominator: Being Shot Up<br />

Sea Dragon<br />

Matching Graph Letter<br />

____________________________<br />

____________________________<br />

____________________________<br />

____________________________<br />

____________________________<br />

____________________________<br />

____________________________<br />

____________________________<br />

____________________________<br />

____________________________<br />

Analysis<br />

1. Write a brief statement that describes your reasoning for selecting the graph you<br />

did for Thunderhawk? Were there specific details on the graph that made you 100%<br />

sure that this graph was the graph for Thunderhawk?<br />

____________________________________________________________________________________<br />

____________________________________________________________________________________<br />

________________________________________________<br />

2. Which graphs to rides interpretations were the hardest to make? For what reasons<br />

were they the most difficult?<br />

____________________________________________________________________________________<br />

____________________________________________________________________________________<br />

________________________________________________<br />

3. Which rides had the most similar graphs? Why do you think they have similar<br />

graphs?<br />

____________________________________________________________________________________<br />

____________________________________________________________________________________<br />

____________________________________________________________________________________<br />

____________________________________<br />

4. On graph I, what trend do you notice about the G forces when the altitude is at its<br />

peak versus when the altitude has reached its low point?<br />

____________________________________________________________________________________<br />

____________________________________________________________________________________<br />

____________________________________________________________________________________<br />

_________________________________<br />

102


Possessed<br />

Preliminary Data:<br />

Your weight in pounds = ________________lb X 4.45 N/lb = ___________________N<br />

weight in Newtons<br />

Your mass, m in kilograms =<br />

___________________kg<br />

2<br />

9.8m<br />

sec<br />

Mass of loaded train = 13,065 kg<br />

Length of the train = 15.75 m<br />

Measure the time it takes for the train to do its first launch (L1) from rest. Suggestion: Use the center of<br />

the train as your reference point. This is the time it takes the train to be accelerated by the LIMs (linear<br />

induction motors). You may want to stand back from the ride to get a better overall view of the station to<br />

take your measurements.<br />

tL1 = ____________________sec<br />

Measure the time it takes for the train to pass through the second boost which is the same time it takes to<br />

pass through the station after the first launch.<br />

here (x = 60 m) here<br />

tL2 = ____________________sec<br />

103


Possessed<br />

Measure the time it takes for the train to pass through the first braking pass in the station.<br />

tB1 = ____________________sec<br />

Measure the time it takes for the train to pass through the second braking pass in the station.<br />

tB2 = ____________________sec<br />

Section 1: Linear Acceleration<br />

1. Since the distance that the train is traveling during its first launch is 48 m and the train starts from<br />

rest, use the linear equation given to calculate the average constant acceleration of the first launch.<br />

Remember that you measured the time.<br />

1 2<br />

x v<br />

i t at<br />

2<br />

Acceleration of the launch, a = ____________________m/sec 2 .<br />

2. Assuming no friction, calculate the average net force you experience.<br />

Favg = ma _______________________N<br />

3. Calculate the average amount of work the LIM’s do on you during the launch knowing the<br />

distance traveled during the launch given in #1.<br />

W = Fdcos______________________J<br />

4. Calculate your force factor you experience while launching.<br />

104


Possessed<br />

ff =<br />

F avg<br />

weight<br />

______________________<br />

5. Using a linear equation given, calculate the speed of the train upon reaching the vertical section<br />

of the track.<br />

2 2<br />

v v 2ax<br />

OR v v at<br />

f<br />

i<br />

f<br />

i<br />

vL1 = _________________________m/sec<br />

6. For the students with the CENCO lateral accelerometers, get in line and ride POSSESSED.<br />

While in line, secure and familiarize yourself with the lateral accelerometer. When on the ride,<br />

have your lateral (horizontal) accelerometer ready for launch. Position the accelerometer as<br />

instructed by your teacher. Measure the average lateral force factor of the first launch by<br />

recording the average location of the BB’s in the tube.<br />

ff = ____________________<br />

Alt. 6. For students with the PASCO or handmade lateral accelerometers, get in line and ride<br />

POSSESSED. While in line, secure and familiarize yourself with your version of the inclinometer (used<br />

as a lateral accelerometer). When on the ride, have your inclinometer ready for launch. Position the<br />

accelerometer as instructed by your teacher. Measure the average angle of the first launch.<br />

Calculate the accelerating force, FN on you by using the following:<br />

θ<br />

θ<br />

Fnety = may<br />

FN cosθ – w = may<br />

FN cosθ – w = 0<br />

FN cosθ = w<br />

w<br />

Calculate your force factor while launching.<br />

ff =<br />

F N<br />

weight<br />

_____________________<br />

Compare your results with that calculated in #4 elaborating on reasons for errors.<br />

105


Possessed<br />

Section 2: Work/Energy considerations for the Launch and Boost<br />

7. Using the conservation of energy and the speed of the train after the initial launch found in<br />

procedure 5, calculate the height of the train on the spiral section of the track.<br />

KEL1 = PEvert.<br />

1<br />

mv<br />

2<br />

<br />

2<br />

L1<br />

mgh vert<br />

h = _________________________m<br />

8. Using the work/energy theorem and the values found in #6, calculate the average amount of work<br />

the LIM’s do on you during the first launch using the<br />

W<br />

LIM<br />

WLIM = KE<br />

1 2 1<br />

mvL<br />

1<br />

mvi<br />

2 2<br />

2<br />

W = _______________________J<br />

9. Now calculate the average amount of work the LIM’s do on the train during the first launch.<br />

WLIM = KE<br />

1 2 1 2<br />

WLIM<br />

mvL<br />

1<br />

mvi<br />

2 2<br />

W = _______________________J<br />

106


Possessed<br />

10. Calculate the average power delivered by the LIMs to the train during the first launch.<br />

P =<br />

W<br />

t L1<br />

_______________________W<br />

OPTIONAL: 11. Calculate the average current supplied by the LIMs during the launch. The voltage<br />

provided to each LIM during launch is 240 V and assuming there are 4 LIMs operating at any given time.<br />

(NOTE: This is an over simplified version as to what actually is occurring electrically during the<br />

launch.)<br />

P = current x voltage<br />

Current = _______________________amperes<br />

12. Assuming no friction, the speed of the train at the end of the first launch must the same as the<br />

speed of the train at the beginning of the second boost because of the conservation of energy.<br />

Knowing the speed of the train at the end of the first launch given in procedure 5, the distance<br />

(xL2 = 60.0 m) of the train during the boost (see picture on page 1), and the time it takes for the<br />

second boost from the initial data, calculate the acceleration and speed of the train after the<br />

second boost using the given linear equation.<br />

1 2<br />

xL2<br />

vL<br />

1t<br />

at AND vL2<br />

vL<br />

1<br />

at<br />

2<br />

aL2 = _________________________m/sec 2 and vL2 = _____________________m/sec<br />

12. Using the work energy theorem, calculate the average amount of work on the train to accelerate it<br />

through the second boost.<br />

WLIM = KE<br />

1 2 1 2<br />

WLIM<br />

mvL2<br />

mvL<br />

1<br />

2 2<br />

W = _______________________J<br />

13. Calculate the average net force on the train for the second boost using the equation.<br />

107


Possessed<br />

F<br />

ma<br />

OR<br />

W F( 2)cos<br />

net<br />

x L<br />

F = _______________________N<br />

14. Compare the force of the second boost to that of the first launch. Are they same or different and<br />

why?<br />

15. Using the conservation of energy and the speed of the train after the second boost, calculate the<br />

height of the train on the straight vertical section of the track.<br />

KEL1 = PEvert.<br />

1<br />

mv<br />

2<br />

<br />

2<br />

L2<br />

mgh vert<br />

h = _________________________m<br />

108


Possessed<br />

Section 3: The Vertical Braking<br />

The train gets stopped for 1 second by standard mechanical clamp brakes when it reaches its highest<br />

point of approximately 37 m as measured from the center of the train on the straight vertical section of<br />

the track.<br />

16. How energy does the train have while held<br />

stationary by these brakes at this height?<br />

PE train<br />

mgh<br />

W = ________________________J<br />

17. How much power is delivered by the brakes at this<br />

point?<br />

PEtrain<br />

P <br />

t<br />

P = _________________________W<br />

18. How much force must the brakes be applying to the train to keep it held in this vertical position?<br />

Force = ________________________N<br />

Section 4: Stopping the train at the end of the ride<br />

19. Using the conservation of energy, calculate the speed of the train upon entering the station after<br />

the vertical brake.<br />

PE KE<br />

mgh<br />

vert.<br />

brake<br />

vert.<br />

brake<br />

<br />

1<br />

2<br />

station<br />

mv<br />

2<br />

station<br />

109


Possessed<br />

vstation = ___________________________m/sec<br />

20. You know the distance and the time, tB1, for the train to pass through the braking pass while<br />

passing through the station. You also know how fast the train is moving upon entering the station<br />

along with the initial speed upon entering the station from procedure 19. Calculate the<br />

acceleration and speed of the train at the end of the first braking pass through the station by using<br />

the equations.<br />

1 2<br />

xstation<br />

vstationt<br />

at AND vB<br />

1<br />

vstation<br />

at<br />

2<br />

aB1 = _____________________m/sec 2 and vB1 = _______________________m/sec<br />

21. Calculate the amount of work required to slow the train in the first braking pass.<br />

W<br />

LIM<br />

WLIM = KE<br />

1 2 1<br />

mvB<br />

1<br />

mv<br />

2 2<br />

2<br />

station<br />

WB1 = ________________________J<br />

22. Calculate the average force the LIMs apply to the train to slow it down during the first braking<br />

pass.<br />

ma OR W F( x)cos<br />

F net<br />

Favg = __________________________N<br />

110


Possessed<br />

23. Since the train stops during it second braking pass through the station, calculate the amount of<br />

work required to slow the train in the second braking pass.<br />

WLIM = KE<br />

1<br />

WLIM<br />

mv<br />

2<br />

2<br />

0<br />

B1<br />

WB2 = ________________________J<br />

24. Calculate the average force the LIMs apply to the train to slow it down during the second braking<br />

pass.<br />

W F x<br />

cos<br />

<br />

Favg = __________________________N<br />

25. Compare the work done or force applied by the LIMs to launch the train at the beginning of the<br />

ride to that in braking the train. Be sure to explain your reasoning.<br />

111


Possessed<br />

Section 4: Vertical Sections of the Ride<br />

. In this section of the lab, you will be looking at the vertical sections of the track to see if the spiral<br />

vertical section of the track affects freefall. Secure the vertical accelerometer as shown in the<br />

diagram below. This orientation is for when you are on the spiral vertical section of the track.<br />

Reverse the accelerometer for the straight vertical section of the track. You will need to orient the<br />

accelerometer so that the weight hangs suspended by the spring when the train is on these sections<br />

of the track.<br />

Spiral side<br />

straight side<br />

When the train is at the highest on these sections of the track, record the force factor. Be sure you<br />

are not recording the force factor while the train is being stopped on the straight vertical section of<br />

the track.<br />

If you do not have a vertical accelerometer, you can use a stopwatch to measure the time it takes<br />

for the train to freefall on these sections.<br />

Vertical Spiral section of track<br />

ffspiral or time = ________________<br />

Vertical straight section of track<br />

ffstraight or time =________________<br />

112


Possessed<br />

Explain any differences in the force factor on these two sections of track. Should there be a difference?<br />

Why or why not?<br />

Section 5: The Upward Curved Sections and Centripetal Force<br />

In this section of the lab you will calculate the radius of each vertical curve by using the force factors<br />

and speeds that you measure. This section can be done as a stand-alone activity or can utilize the<br />

data from the previous sections. You can use the speeds from the previous sections. It would be<br />

helpful if you have several students taking measurements at the same time.<br />

Measure the time the train takes to pass the lone vertical support post outside of the station on each side<br />

of the station shown in the picture. If time permits, measure the speed at these points for one,<br />

two, or three passes. The more data you have, the more accurate your calculations. Enter the data<br />

into the table below.<br />

By knowing the length of the train given in the preliminary data at the beginning of the lab, calculate the<br />

speed of the train just as it enters the vertical curves. Enter the data in the table below.<br />

Secure the vertical accelerometer and measure the force factor you experience while passing through the<br />

curves for each pass you predetermined. Be sure you are measuring the force factor that<br />

corresponds to the time you measured. Also, be sure that you are holding the vertical<br />

accelerometer parallel to your body as shown in the picture on the next page.<br />

113


Possessed<br />

Pass<br />

time<br />

(sec)<br />

Spiral side<br />

speed<br />

(m/sec)<br />

force<br />

factor<br />

radius<br />

(m)<br />

time<br />

(sec)<br />

Vertical Side<br />

speed<br />

(m/sec)<br />

force<br />

factor<br />

radius<br />

(m)<br />

1<br />

2<br />

3<br />

According to the free-body diagram and the two expressions given,<br />

Fseat<br />

ac<br />

F<br />

ff <br />

w<br />

F<br />

seat<br />

seat<br />

w <br />

mv<br />

r<br />

2<br />

w<br />

1. Derive an expression for calculating the radius of curvature of the track.<br />

2. Calculate the radius of curvature for each curve and enter the data into the table on the<br />

previous page.<br />

QUESTIONS:<br />

1. Compare the radius on the straight side and the spiral side of the ride.<br />

114


Possessed<br />

2. As the speed increased, explain what happened to the force factor.<br />

3. As the speed increased, explain what happened with the radius?<br />

4. If the radius was smaller, what would happen to the force factor? Speed? Support your answer.<br />

115


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Unifying Themes<br />

Academic<br />

Standard<br />

Standard<br />

Category<br />

3.1.10 C<br />

Standard<br />

Statement<br />

C. Apply<br />

patterns as<br />

repeated<br />

processes or<br />

recurring<br />

elements in<br />

science and<br />

technology.<br />

Content<br />

Descriptors<br />

Examine and<br />

describe physical<br />

patterns in motion.<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Antique Carrousel<br />

Apollo 2000<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water<br />

Landing<br />

Unifying<br />

Themes<br />

3.1.10 D<br />

3.1.12 C<br />

3.1.12 D<br />

D. Apply scale as a<br />

way of relating<br />

concepts and<br />

ideas to one<br />

another by<br />

some measure.<br />

C. Assess and<br />

apply patterns in<br />

science and<br />

technology.<br />

D. Analyze scale as<br />

a way of relating<br />

concepts and<br />

ideas to one<br />

another by<br />

some measure.<br />

Apply dimensional<br />

analysis and scale as a<br />

ratio.<br />

Assess and apply<br />

recurring patterns<br />

in natural and<br />

technological<br />

systems.<br />

Compare and<br />

contrast structure and<br />

function relationships<br />

as they relate to<br />

patterns.<br />

Assess patterns in<br />

nature using<br />

mathematical<br />

formulas.<br />

Assess the use of<br />

several units of<br />

measurement to the<br />

same problem.<br />

Analyze and apply<br />

appropriate<br />

measurement scales<br />

when collecting data.<br />

Antique Carrousel<br />

Dominator<br />

Enterprise<br />

Sea Dragon<br />

Steel Force<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

116


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Inquiry and Design<br />

Academic<br />

Standard<br />

Standard<br />

Category<br />

3.2.7 A<br />

3.2.4 B<br />

Standard<br />

Statement<br />

A. Explain and apply<br />

scientific and technological<br />

knowledge.<br />

B. Describe objects in the<br />

world using the<br />

five senses.<br />

Content<br />

Descriptors<br />

Answer “What if” questions based<br />

on observation, inference or prior<br />

knowledge or experience.<br />

Recognize observational<br />

descriptors from each of the five<br />

senses (e.g., see-blue, feel-rough).<br />

Use observations to develop a<br />

descriptive vocabulary.<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

Inquiry and<br />

Design<br />

3.2.7 B<br />

3.2.10 B<br />

B. Apply process<br />

knowledge to make and<br />

interpret observations.<br />

B. Apply process<br />

knowledge and organize<br />

scientific and<br />

technological phenomena<br />

in varied ways.<br />

Measure materials using a variety<br />

of scales.<br />

Describe relationships by making<br />

inferences and predictions.<br />

Communicate, use space / time<br />

relationships, define operationally,<br />

raise questions, formulate<br />

hypotheses, test and experiment,<br />

Design controlled experiments,<br />

recognize variables, manipulate<br />

variables.<br />

Interpret data, formulate models,<br />

design models, and produce<br />

solutions.<br />

Develop appropriate scientific<br />

experiments: raising questions,<br />

formulating hypotheses, testing,<br />

controlled experiments, recognizing<br />

variables, manipulating variables,<br />

interpreting data, and producing<br />

solutions.<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

117


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Inquiry and Design<br />

Academic<br />

Standard<br />

Inquiry and<br />

Design<br />

Standard<br />

Category<br />

3.2.12 B<br />

3.2.10 C<br />

3.2.12 C<br />

Standard<br />

Statement<br />

B. Evaluate experimental<br />

information for<br />

appropriateness and<br />

adherence to<br />

relevant science<br />

processes.<br />

C. Apply the elements of<br />

scientific inquiry to solve<br />

problems.<br />

C. Apply the elements of<br />

scientific inquiry to solve<br />

multi-step problems.<br />

Content<br />

Descriptors<br />

Evaluate experimental data<br />

correctly within experimental<br />

limits.<br />

Judge that conclusions are<br />

consistent and logical with<br />

experimental conditions.<br />

Interpret results of experimental<br />

research to predict new information<br />

or improve a solution.<br />

Generate questions about objects,<br />

organisms and/or events that can be<br />

answered through scientific<br />

investigations.<br />

Evaluate the appropriateness of<br />

questions.<br />

Conduct a multiple step<br />

experiment.<br />

Organize experimental information<br />

using a variety of analytic methods.<br />

Judge the significance of<br />

experimental information in<br />

answering the question.<br />

Suggest additional steps that might<br />

be done experimentally.<br />

Generate questions about objects,<br />

organisms and/or events that can be<br />

answered through scientific<br />

investigations.<br />

Evaluate the appropriateness of<br />

questions.<br />

Organize experimental information<br />

using analytic and descriptive<br />

techniques.<br />

Evaluate the significance of<br />

experimental information in<br />

answering the question.<br />

Project additional questions from a<br />

research study that could be studied.<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

118


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Inquiry and Design<br />

Academic<br />

Standard<br />

Standard<br />

Category<br />

Standard<br />

Statement<br />

Content<br />

Descriptors<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Inquiry and<br />

Design<br />

3.2.10 D<br />

3.2.12 D<br />

D. Identify and apply the<br />

technological design<br />

process to solve<br />

problems.<br />

D. Analyze and use the<br />

technological design<br />

process to solve<br />

problems.<br />

Examine the problem, rank all<br />

necessary information and all<br />

questions that must be answered.<br />

Assess all aspects of the problem,<br />

prioritize the necessary information<br />

and formulate questions that must<br />

be answered.<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

119


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Physical Science<br />

Academic<br />

Standard<br />

Standard<br />

Category<br />

Standard<br />

Statement<br />

Content<br />

Descriptors<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Physical<br />

Science<br />

3.4.4 C<br />

C. Observe and<br />

describe different<br />

types of force and<br />

motion.<br />

Describe various<br />

types of motions.<br />

Compare the relative<br />

movement of<br />

objects and describe<br />

types of motion<br />

that are evident.<br />

Describe the<br />

position of an object<br />

by locating it relative<br />

to another object or<br />

the background (e.g.,<br />

geographic direction,<br />

left, up).<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

3.4.7 C<br />

C. Identify and<br />

explain the<br />

principles of force<br />

and motion.<br />

Explain various<br />

motions using models.<br />

<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

120


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Physical Science<br />

Academic<br />

Standard<br />

Physical<br />

Science<br />

Standard<br />

Category<br />

3.4.10 C<br />

3.4.12 C<br />

Standard<br />

Statement<br />

C. Distinguish<br />

among the<br />

principles of force<br />

and motion.<br />

C. Apply the<br />

principles of motion<br />

and force.<br />

Content<br />

Descriptors<br />

Know Newton’s laws<br />

of motion<br />

(including inertia,<br />

action and<br />

reaction) and gravity<br />

and apply them to<br />

solve problems<br />

related to forces and<br />

mass.<br />

Determine the<br />

efficiency of<br />

mechanical systems<br />

by applying<br />

mathematical<br />

formulas, concepts<br />

through words,<br />

models and<br />

mathematical<br />

symbols.<br />

Analyze the<br />

principles of<br />

translational motion,<br />

velocity and<br />

acceleration as they<br />

relate to free fall and<br />

projectile motion.<br />

Analyze the<br />

principles of<br />

rotational motion to<br />

solve problems<br />

relating to angular<br />

momentum, and<br />

torque.<br />

Interpret a model<br />

that illustrates<br />

circular motion and<br />

acceleration.<br />

Describe inertia,<br />

motion, equilibrium,<br />

and action/reaction<br />

concepts through<br />

words, models and<br />

mathematical<br />

symbols.<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

121


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Technological Devises<br />

Academic<br />

Standard<br />

Technological<br />

Devises<br />

Standard<br />

Category<br />

3.7.7 A<br />

3.7.7 B<br />

3.7.10 A<br />

Standard<br />

Statement<br />

A. Describe the<br />

safe and<br />

appropriate use of<br />

tools, materials<br />

and techniques to<br />

answer questions<br />

and solve<br />

problems.<br />

B. Use appropriate<br />

instruments and<br />

apparatus to study<br />

materials.<br />

A. Identify and<br />

safely use a variety<br />

of tools, basic<br />

machines, materials<br />

and techniques to<br />

solve problems and<br />

answer questions.<br />

Content<br />

Descriptors<br />

Identify uses of<br />

tools, machines,<br />

materials,<br />

information, people,<br />

money, energy and<br />

time that meet specific<br />

design criteria.<br />

Describe safe<br />

procedures for using<br />

tools and materials.<br />

Assess materials for<br />

appropriateness of<br />

use.<br />

Select appropriate<br />

instruments to<br />

measure the size,<br />

weight, shape and<br />

temperature of living<br />

and non-living<br />

objects.<br />

Apply knowledge of<br />

different<br />

measurement systems<br />

to measure<br />

and record objects’<br />

properties.<br />

Select and safely<br />

apply appropriate<br />

tools, materials and<br />

processes necessary<br />

to solve complex<br />

problems.<br />

Apply advanced tool<br />

and equipment<br />

manipulation<br />

techniques to solve<br />

problems.<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

122


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Technological Devises<br />

Academic<br />

Standard<br />

Technological<br />

Devises<br />

Standard<br />

Category<br />

3.7.10 B<br />

3.7.12 A<br />

Standard<br />

Statement<br />

B. Apply<br />

appropriate<br />

instruments and<br />

apparatus to<br />

examine a variety<br />

of objects and<br />

processes.<br />

A. Apply advanced<br />

tools, materials<br />

and<br />

techniques to<br />

answer complex<br />

questions.<br />

Content<br />

Descriptors<br />

Describe and use<br />

appropriate<br />

instruments to gather<br />

and analyze data.<br />

Compare and<br />

contrast different<br />

scientific<br />

measurement<br />

systems; select the<br />

best measurement<br />

system for a specific<br />

situation.<br />

Explain the need to<br />

estimate<br />

measurements within<br />

error of various<br />

instruments.<br />

Apply accurate<br />

measurement<br />

knowledge to solve<br />

everyday problems.<br />

Select and safely<br />

apply appropriate<br />

tools, materials and<br />

processes necessary<br />

to solve complex<br />

problems that could<br />

result in more than<br />

one solution.<br />

Evaluate and use<br />

technological<br />

resources to solve<br />

complex multi-step<br />

problems.<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

123


Coaster Quest<br />

Pennsylvania Standards in Science and Technology<br />

Technological Devises<br />

Academic<br />

Standard<br />

Technological<br />

Devises<br />

Standard<br />

Category<br />

3.7.12 B<br />

Standard<br />

Statement<br />

B. Evaluate<br />

appropriate<br />

instruments and<br />

apparatus to<br />

accurately<br />

measure<br />

materials and<br />

processes.<br />

Content<br />

Descriptors<br />

Apply and evaluate<br />

the use of<br />

appropriate<br />

instruments to<br />

accurately measure<br />

scientific and<br />

technologic<br />

phenomena within the<br />

error limits of the<br />

equipment.<br />

Evaluate the<br />

appropriate use of<br />

different<br />

measurement scales<br />

(macro and micro).<br />

Evaluate the utility<br />

and advantages<br />

of a variety of absolute<br />

and relative<br />

measurement scales<br />

for their appropriate<br />

application.<br />

Performance<br />

Tasks and<br />

Associated<br />

Learning<br />

Activities<br />

Antique Carrousel<br />

Apollo 2000<br />

Dominator<br />

Enterprise<br />

Ferris Wheel<br />

Revolution<br />

Sea Dragon<br />

Steel Force<br />

Wave Swinger<br />

White Water Landing<br />

124

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