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TAM 212 Worksheet 3 Solutions

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Name: Group members:<br />

<strong>TAM</strong> <strong>212</strong> <strong>Worksheet</strong> 3<br />

<strong>Solutions</strong><br />

This worksheet is concerned with designing the track for the Chicago O’Hare Airport Transit System (ATS):<br />

We want to design one curve on the track between two perpendicular straight line segments. One easy option<br />

would be to use a quarter-circle:<br />

direction of travel<br />

1<br />

O<br />

r = 100 m<br />

θ<br />

êθ<br />

P<br />

êr


1. If the train moves around the track at constant speed v = 10 m/s, what is its angular velocity ω about O<br />

while on the circular segment?<br />

ω = 0.1 rad/s<br />

2. Plot the radial ar and angular aθ components of the train’s acceleration a = ar êr + aθ êθ versus θ as the<br />

train moves around the circular segment. Clearly mark all significant points on the vertical axis.<br />

1<br />

0<br />

1<br />

ar<br />

Π<br />

4<br />

Π<br />

2<br />

Θ<br />

3. On airport trains people are normally standing. As the lead engineer for the ATS system design, do you<br />

anticipate any problems for the passengers on this train as it goes along this track?<br />

The radial acceleration will suddenly jump from zero on the straight-line segments to −1 m/s 2 on the curve.<br />

This will be uncomfortable for the passengers who will feel this as a sudden jerk sideways.<br />

4. To give the passengers a smoother ride, we want to make the track have a radius r that varies with the<br />

angle θ, so r = r(θ), while still keeping a constant angular velocity ˙ θ = ω. Use the chain rule to find ˙r and<br />

¨r and so write the acceleration in the polar basis in terms of r ′ (θ), r ′′ (θ) and ω. Here r ′ (θ) is the derivative<br />

with respect to θ.<br />

The chain rule gives ˙r = r ′ ˙ θ and ¨r = r ′′ ˙ θ 2 + r ′ ¨ θ. Also ˙ θ = ω and ¨ θ = 0, so<br />

a = (¨r − r ˙ θ 2 )êr + (r ¨ θ + 2 ˙r ˙ θ)êθ = (r ′′ − r)ω 2 êr + 2r ′ ω 2 êθ<br />

2<br />

1<br />

0<br />

1<br />

aΘ<br />

Π<br />

4<br />

Π<br />

2<br />

Θ


5. From now on we will keep ω fixed at the constant value from Question 1 and we will use the functional<br />

form:<br />

<br />

2<br />

r(θ) = Aθ θ − π<br />

2 + 100 m<br />

2<br />

where θ is in radians and A is an unknown constant. This function looks like:<br />

100<br />

r<br />

0<br />

0<br />

Π<br />

4<br />

Using this function, what are the radial and angular components of the acceleration when the train just<br />

enters the curved track segment?<br />

Evaluating the above acceleration expression with this r(θ) gives:<br />

<br />

2<br />

r(θ) = Aθ θ − π<br />

2<br />

r ′ <br />

(θ) = 2Aθ θ − π<br />

r ′′ <br />

(θ) = 2A θ − π<br />

2<br />

The acceleration at θ = 0 is thus:<br />

2<br />

2<br />

2<br />

2<br />

+ 100 r(0) = 100<br />

<br />

2<br />

+ 2Aθ θ − π<br />

<br />

2<br />

r ′ <br />

+ 8Aθ θ −<br />

(0) = 0<br />

π<br />

<br />

+ 2Aθ<br />

2<br />

2<br />

r ′′ (0) = Aπ2<br />

2<br />

2 Aπ<br />

a =<br />

200<br />

ar = Aπ2<br />

− 1<br />

200<br />

aθ = 0<br />

<br />

− 1 êr<br />

6. What value of A will give an acceleration profile that does not abruptly jump when moving onto the curve<br />

from the straight-line segment?<br />

To have zero initial acceleration on the curve we need A = 200/π 2 ≈ 20.3 m.<br />

3<br />

Π<br />

2<br />

Θ

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