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Understanding RL Circuits (Lab 9)

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Goals:<br />

<br />

<br />

<br />

<strong>RL</strong> <strong>Circuits</strong><br />

To quantify the rate at which the potential difference across an inductor changes when<br />

connected in series with a resistive element.<br />

To discuss differences in the behaviors of a circuit with only a resistive element, a circuit<br />

with a capacitor in series with a resistive element, and a circuit with an inductor and a<br />

resistive element.<br />

To practice linearization of data as a data-analysis technique.<br />

Equipment:<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

Science Workshop Interface<br />

Voltage Probes<br />

Digital Multimeter (DMM)<br />

Phys212 <strong>Lab</strong>Kit Module<br />

<strong>RL</strong>C circuit board<br />

5 and Diode Circuit board<br />

High inductance coil<br />

(7) Stackable banana-plug connecting wires<br />

(4) Alligator connecting wires<br />

Software: Microsoft Excel, DataStudio<br />

Introduction:<br />

In an earlier lab, we examined how capacitors and resistors interact in a circuit. In this lab, we<br />

will study how indutors and resistors interact in a circuit (called an <strong>RL</strong> Circuit). We will<br />

approach this qualitatively and then quantitatively.<br />

Due to Faraday’s Law, inductors oppose changes in the current through them. Any change in<br />

current changes the magnetic field created by the inductor which means that the magnetic flux<br />

through the inductor changes. This change in flux induces an EMF to oppose the change. The<br />

induced EMF, induced , of an inductor is given by:<br />

di<br />

<br />

induced<br />

L<br />

(Eq. 1)<br />

dt<br />

di<br />

where L is inductance, and i is the current through the inductor (so is the rate of change of the<br />

dt<br />

current). The negative sign comes from the fact that this induced EMF creates a magnetic field<br />

which opposes the change in flux. A capacitor’s capacitance depends how it was made (i.e. size<br />

/ shape of the terminals, how they are separated, what material is between them), and a resistor’s<br />

resistance depends how it was made (i.e. what material it was made of and what shape it is). The<br />

inductance of an inductor is given by:<br />

<br />

B<br />

N L B-one<br />

(Eq. 2)<br />

i i


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 2<br />

where B is the magnetic flux through the inductor. This magnetic flux is the flux created<br />

through the inductor by the current which passes through it (this is why inductance is more<br />

properly called “self-inductance”). The inductors we encounter are often made of many turns of<br />

wire and so it can be useful to note that the magnetic flux could be looked at as the magnetic flux<br />

created by one turn of wire ( B-one ) multiplied by the number of turns of wire (N) making the<br />

inductor. In other words, the more turns of wire an inductor has, the larger its inductance will be.<br />

The inductance can also be increased by placing a ferromagnetic material within the center of the<br />

inductor. The magnetic field created by the inductor in the current will magnetize this core; as<br />

the inductor’s magnetic field changes so will the magnetization of the core. This in turn will<br />

correspond to a larger change in flux.<br />

When an inductor is connected in series with a resistor of resistance R and a power supply or<br />

battery with EMF , the inductor will oppose any change in flux (by trying to keep the current at<br />

its initial value, zero). This will cause the voltage across the inductor to spike. The voltage<br />

across the inductor then decays with time. As the inductor opposes the change in current, the<br />

current will increase rapidly at first, then the rate at which the current changes will decrease as it<br />

eventually reaches a final steady-state value. This process is described by the equations<br />

<br />

<br />

<br />

t<br />

i t 1 e <br />

<br />

<br />

(Eq. 3)<br />

R <br />

and<br />

V<br />

L<br />

t<br />

<br />

t<br />

<br />

e<br />

(Eq. 4)<br />

As with an RC circuit, the quantity t is called the time constant of the circuit. For an <strong>RL</strong> circuit,<br />

the time constant is given by<br />

L<br />

<br />

(Eq. 5)<br />

R<br />

If an inductor has a current through it and then is removed from the battery in such a way that it<br />

is still connected to a resistance R, the inductor will still oppose any change in flux (by trying to<br />

keep the current at its initial value and direction, whatever those are). The current through the<br />

inductor will decrease rapidly but then the rate will slow as it approaches zero. This process is<br />

described by the equations<br />

t<br />

<br />

it<br />

e<br />

(Eq. 4)<br />

R<br />

and<br />

V<br />

L<br />

t<br />

<br />

t<br />

<br />

e<br />

(Eq. 5)


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 3<br />

Name: ____________________________<br />

Name: ____________________________<br />

Name: ____________________________<br />

Date: ______________<br />

<strong>Lab</strong> Sect.: __________<br />

<strong>Lab</strong> Instructor: ______________________<br />

Directions:<br />

<strong>Lab</strong> Activity 1: Charging and Discharging of <strong>RL</strong> Circuit<br />

Construct the circuit shown in Figure 1 below. Make sure that you connect the batteries<br />

to each other with the correct polarities (i.e., the positive end of one battery connected to<br />

the negative terminal of the second battery). The resistor in the circuit is the round bulb<br />

on the same circuit board as the switch. The switch has two possible closed positions,<br />

labeled A and C. Position A requires the switch to be held to keep it closed. Because we<br />

do not want to accidentally leave the batteries connected to the circuit, in this lab, we will<br />

only use position A. Also make sure that the light bulbs are properly screwed into their<br />

sockets.<br />

A<br />

B<br />

C<br />

Figure 1 A circuit with two batteries and a light bulb. Please ask your teaching assistants if you<br />

are unsure about your wiring of the circuit.<br />

<br />

Throw the switch to A for a few moments and observe the light bulb. Throughout this<br />

lab, wait at least thirty seconds between runs to ensure that the light bulb cools.<br />

Q1. What happens to the light bulb when the switch is thrown to A (this is not a trick question,<br />

just describe what happens)?<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 4<br />

Q2. What happened to the light bulb in an RC circuit (look back at “<strong>Understanding</strong> RC <strong>Circuits</strong>”<br />

if you can’t recall)?<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

.<br />

<br />

<br />

<br />

<br />

<br />

<br />

<br />

Open DataStudio (start → Programs → DataStudio → DataStudio), and click on<br />

Create Experiment.<br />

Click on Add Sensor or Instrument.<br />

Select Voltage Sensor<br />

Click and drag the Graph icon onto the Voltage Sensor icon.<br />

Click and drag the Table icon shown above to Voltage Sensor icon.<br />

You should feel free to arrange the displays as you see fit. After doing this, your screen<br />

should display the Graph and Table display.<br />

Change the sample rate for the Voltage Sensor from 10 Hz to at least 4,000 Hz. The<br />

changes we will record have a very short time scale; the Science Workshop 750 Interface<br />

has a maximum sample rate of 250,000 Hz when using a single analog sensor.<br />

<br />

Modify the circuit to be the one shown in Figure 2 below. One of the two inductors, is on<br />

the “<strong>RL</strong>C Circuit” board and the other is the “High Inductance Coil” attached to the<br />

wooden board. Some things to keep in mind while you are constructing this circuit:<br />

o The <strong>RL</strong>C Circuit board has wires embedded in it (the white lines show where they<br />

are). To connect the inductor (the spool of wire), insert one banana plug wire into<br />

the socket on either side of the inductor. Remove the metal bar from the <strong>RL</strong>C<br />

Circuit board and insert it into the center of the inductor. This will increase its<br />

inductance.<br />

o To ensure a good connection for the High inductance coil, connect an alligator<br />

clip to both of the two brass posts sticking out of the wooden board. Connect the<br />

other ends of the alligator clips’ wires to banana plugs to be used with the circuit<br />

boards.<br />

o Do NOT close the circuit yet (i.e., leave the switch in the open position B).


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 5<br />

A<br />

B<br />

C<br />

Figure 2 An <strong>RL</strong> charging circuit. Please ask your teaching assistants if you are unsure about your wiring of the<br />

circuit.<br />

Q3. Why have we asked you to connect the two inductors in series like this? Things to consider<br />

to help answer this: What should connecting the inductors in series do to the total inductance<br />

and why (with physical reasoning, not just quoting an equation)? Why might we want to make<br />

that effect to the total inductance (look back at the <strong>RL</strong> circuit equations)?<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 6<br />

Q4. Predict what will happen to the voltage across the inductors after you close the switch to A<br />

and then release the switch. Sketch (qualitatively) below what you expect the time variation of<br />

the voltage to look like including what should happen after the switch is released. <strong>Lab</strong>el the point<br />

at which you would release the switch from A. (Alternatively, you can make a graph using Excel<br />

and attach it to your lab report, if you so wish.) Explain why you drew those forms.<br />

DV L<br />

t<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 7<br />

Q5. Now, actually throw the switch to A for a few moments and observe the light bulb.<br />

Describe (qualitatively) what happens to the light bulb when you move the switch to position A<br />

(including any differences between this circuit and the one with only a light bulb or an RC<br />

circuit).<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

<br />

<br />

<br />

Connect the voltage probes to measure the voltage V L across the inductors.<br />

Click on the Start button in DataStudio to begin recording data, and close the circuit by<br />

moving the switch to position A.<br />

o When a steady state has been reach, release the switch<br />

o When a new steady state has been reached, stop recording data by clicking the<br />

Stop button in DataStudio.<br />

You might wish to do this a few times in order to get a reasonable set of data. Note that<br />

you can delete any set of data simply by highlighting the name of the data set in the Data<br />

window and then pressing the Delete key.


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 8<br />

Q6. Sketch (qualitatively) the time variation of the measured voltage across the inductors. <strong>Lab</strong>el<br />

the point at which you released the switch from A. (Alternatively, you can print the graph and<br />

attach it to your lab report, if you so wish.) Make sure your graph includes what happened after<br />

the switch was released. If some parts of the behavior, have different time scales than others,<br />

you should include multiple graphs (one for each section of the behavior).<br />

DV L<br />

t<br />

Q7. Discuss any differences between your graph from Data Studio (Q6) and your initial sketch<br />

(Q4). What might have caused them (explain at least one difference between the two graphs; if<br />

there are no differences, then be sure you completely explained all of the features you predicted<br />

above in Q4)?<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 9<br />

Q8. As a reminder, here is what the voltage across a charging and then discharging capacitor<br />

looked like (from the lab “<strong>Understanding</strong> RC <strong>Circuits</strong>”):<br />

DV C<br />

Start Discharging<br />

t<br />

Qualitatively compare and contrast this and what you observed for the inductor. Explain any<br />

differences or similarities. (Hint: Since the inductor opposes changes in current, when it is first<br />

connected, what does it act like? When it is connected for a long time, what does it act like?)<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

Move the voltage probes so that you are measuring the voltage across the light bulb, V R .


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 10<br />

Q10. Attach the graph of measured voltage across the bulb V R vs. t to your lab report. <strong>Lab</strong>el the<br />

point at which you released the switch from A.<br />

Q11. Explain qualitatively why the voltage across the bulb varies as observed. Explain what that<br />

means about the current through the light bulb and so your observations in Q5.<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 11<br />

<strong>Lab</strong> Activity 2: Quantitative Analysis of an <strong>RL</strong> Circuit<br />

In this activity, we’re going to distinguish between V L-total (the total voltage across the inductors<br />

at any time), V L (the voltage across the inductors due to their inductance and a changing current),<br />

and V L - R (the voltage across the inductors due to their resistance). The three are related by:<br />

V L-total = V L + V L-R (Eq. 6)<br />

<br />

<br />

<br />

Modify (re-wire) your circuit so that the 5 resistor on the separate circuit board is used<br />

in place of the light bulb. (Since the resistor is ohmic, we won’t have to worry about any<br />

non-ohmic behavior of the light bulb.)<br />

Repeat the first experiment that you carried out earlier: i.e., record the voltage V L-total<br />

across the inductor as a function of time after you have placed the switch at A<br />

Export the measured data to an Excel spreadsheet for analysis as follows:<br />

o In the Table display, highlight the columns of data containing the time and<br />

voltage readings.<br />

o Copy this to the clipboard (Press Ctrl-C or select Copy from the Edit menu)<br />

o Open Microsoft Excel and start a new spreadsheet.<br />

o Paste (Ctrl-V) the copied data into the first two columns.<br />

o Check the units on the data columns so you can label your graphs properly<br />

Q12. Use Excel to make a graph of V L-total versus t from the point after you moved the switch to<br />

A to just before you released the switch. Remember to label the axes on your graphs correctly<br />

with proper units. Include this graph with your lab report.<br />

Q13. If we rescale the data to remove the steady state voltage (V L-R ), we’ll be able to find the<br />

time constant fairly easily (this is making the approximation that the voltage change due to the<br />

inductors’ resistance is constant which isn’t quite right). Rescale the data and use Excel to make<br />

a graph of V L versus t just between the point when you moved the switch to A and when the<br />

steady state was reached. Remember to label the axes on your graphs correctly with proper<br />

units. Include this graph with your lab report.


PHYS 212 <strong>Lab</strong> <strong>Understanding</strong> <strong>RL</strong> <strong>Circuits</strong> 12<br />

Q14. How would you plot the data in such a way that tests whether it obeys the <strong>RL</strong> circuit<br />

equations? (Note that the easiest type of data to fit is a straight line! So, think about how to<br />

transform the equation into a form that allows you to see whether the data follows a straight line.<br />

Think logarithms! You may need to make new columns in your Excel file) Include this plot with<br />

your report. From the plot, determine the value of the time constant. Explain below how you did<br />

this and include any comments that you can about the size of the time constant. (Include your<br />

new graph.)<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________<br />

_____________________________________________________________________________

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