Capacitor Charge & Discharge (AQA A Level Physics)

Exam Questions

3 hours29 questions
1a3 marks

Figure 1 shows a circuit used to investigate how capacitors store charge. 

Figure 1

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The circuit includes a battery, a capacitor C of capacitance 400 μF, a switch S, an ammeter and a voltmeter. 

When the switch S is closed, label the following on Figure 1

(i)

The direction of electron flow in the circuit 

(ii)

The side of capacitor C that becomes negatively charged with an X 

(iii)

The side of capacitor C that becomes positively charged with a Y.

1b3 marks

When the switch S is closed in the circuit shown in Figure 1, measurements from the ammeter are captured by a data logger. 

On the axes provided below, sketch a graph to show what how the ammeter readings would vary with time. 

Include suitable axes labels on your sketch.

7-7-s-q--q1b-easy-aqa-a-level-physics

1c4 marks

After becoming fully charged, the capacitor C from Figure 1 is then discharged via a two-way switch, T through a resistor R of resistance 5 kΩ. This is shown in Figure 2. 

Figure 2

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(i)

Define the time constant of a capacitor discharging through a resistor

(ii)

Calculate the time constant of the circuit shown in Figure 2

1d2 marks

The resistor in Figure 2 is replaced with different resistor with a resistance ten times greater. 

All other components are kept the same. 

State and explain the effect this has on the time constant of the circuit shown in Figure 2.

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2a2 marks

Isabelle won a national physics competition for an idea she developed, which involves measuring the intensity of light using capacitors and data loggers. 

The circuit she designed consists of a photovoltaic cell, P which can generate a potential difference proportional to the intensity of light incident on it. This is connected to a capacitor C, a switch S and a data logger, shown in Figure 1 below: 

Figure 1

7-7-s-q--q2a-easy-aqa-a-level-physics

Explain why the data logger is connected in parallel across the capacitor C.

2b6 marks

Isabelle’s experiment involved printing measurements from the data logger as shown in Table 1 below. 

Table 1

Time / s

p.d. / mV

ln (p.d. / mV)

0

100

4.6

20

70

4.2

40

48

3.9

60

35

 

80

24

 

100

18

 

Some of the data is not shown in Table 1. 

(i)

Complete the missing data in Table 1 

(ii)

Plot the data from Table 1 on the graph below and draw an appropriate line of best fit

7-7-s-q--q2b-easy-aqa-a-level-physics

2c2 marks

Isabelle’s report included a detailed description of how a graph of the data could be used to verify the capacitance of the capacitor C. 

She proposed the equation of the line as: 

      ln V = – begin mathsize 16px style fraction numerator 1 over denominator R C end fraction end stylet + ln begin mathsize 16px style V subscript 0 end style 

and stated that the quantity RC is known as the time constant of the capacitor.

(i)

State the unit of the quantity RC

(ii)

State the meaning of the quantity represented by begin mathsize 16px style V subscript 0 end style

2d3 marks

Isabelle demonstrated that the gradient of the line she obtained had a value of 0.0165. 

Use the value of Isabelle’s gradient, and the equation of the line in part (c), to calculate the time constant of the capacitor.

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3a2 marks

A capacitor is connected to a power supply such that it is fully charged. 

Figure 1 below shows the variation of the charge Q stored on the capacitor with time t: 

Figure 1

7-7-s-q--q3a-easy-aqa-a-level-physics

Define the time constant for a charging capacitor. 

3b3 marks

The maximum value of the charge from Figure 1 is 1.5 C. 

Use Figure 1 to determine the time constant for the charging capacitor.

3c3 marks

The capacitor stores a maximum charge at a potential difference of 5.0 V. 

Calculate the capacitance of the capacitor. 

State an appropriate unit with your answer.

3d2 marks

The capacitor is then allowed to discharge through a resistor of resistance 100 Ω. 

Using your answer to part (c), calculate the charge that remains on the capacitor after a time of 25 s.

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4a2 marks

When a capacitor is charging, the potential difference V across its plates at a time t can be calculated. 

The capacitor is effectively ‘fully charged’ when the potential difference across its plates is equal to the emf of the power supply.  

Calculate the potential difference across a capacitor of capacitance 10 mF that is connected to a power supply of emf 6.0 V after 30 s. 

            The capacitor charges through a resistor of resistance 5.5 kΩ.

4b2 marks

Calculate how long it takes for the charge stored on the capacitor described in part (a) to reach 63% of its maximum.

4c2 marks

When the capacitor described in part (a) begins its charging process, the current decreases rapidly from an initial value of 0.5 A. 

Calculate the current in the circuit after 55 s.

4d1 mark

Figure 1 shows how the current I varies with time t for a charging capacitor: 

Figure 1

7-7-s-q--q4d-easy-aqa-a-level-physics

State the quantity represented by the area under the line shown in Figure 1.

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5a4 marks

A set of revision notes on capacitance summarises key information about graphs as shown in Table 1 below. 

Table 1

Vertical axis

Horizonal axis

Gradient represents

Area represents

pd

time

n/a

n/a

charge

 

current

n/a

 

time

n/a

charge transferred

charge

pd

 

 

Complete the information in Table 1.

5b3 marks

A parallel plate capacitor of capacitance 100 mF is fully charged. This is shown by the graph of potential difference V against time t in Figure 1 below. 

Figure 1

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Use Figure 1 to calculate the energy stored by this capacitor when it is fully charged.

5c2 marks

The capacitor described in part (b) is now allowed to fully discharge through a fixed 2 Ω resistor. 

Calculate the time constant for the discharging capacitor.

5d2 marks

The capacitor and the resistor described in part (b) is to be used in the circuit for a smartphone’s battery. 

In order to maximise the usage time between charging the smartphone, the capacitor’s manufacturer wishes to increase its time constant when discharging.  

State and explain how the manufacturer should adjust the resistance of the discharging circuit in order to increase the time constant.

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1a3 marks

Figure 1 below shows part of the discharge curve for a capacitor of capacitance 60 µF. 

Figure 1

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The capacitor was initially charged to a potential difference (p.d.) of 1.8 V and then discharged through a resistor. 

Show that the resistance of the resistor is about 130 Ω.

1b3 marks

State and explain how the potential difference changes as the capacitor discharges.

1c3 marks

Calculate the percentage of the initial energy stored by the capacitor that remains after the first 0.012 s of the discharge. 

1d1 mark

Calculate the percentage of the initial energy stored by the capacitor that is lost in the first 0.012 s of the discharge.

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2a3 marks

A capacitor, initially charged to 6.0 V, was discharged through a 500 kΩ resistor. A datalogger was used to record the pd across the capacitor at frequent intervals. The graph in Figure 1 shows how the pd varied with time during the first 20 s of discharge. 

 Figure 1

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Use Figure 1 to determine the time constant of the circuit, giving an appropriate unit.

2b2 marks

Hence, calculate the capacitance of the capacitor in µF.

2c3 marks

Show that the capacitor's energy drops to about 70% of its initial energy stored after about 2 s.

2d3 marks

A camera flash contains a capacitor identical to the capacitor used in part (a). It is charged from an 18 V supply and then discharged through a 500 kΩ resistor.

State and explain the effect of this higher initial p.d. on: 

(i)
The energy stored by the capacitor initially. 
(ii)
The time taken for the capacitor to drop to 70% of its original energy.

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3a2 marks

A capacitor is charged to a maximum of 13.2 µC with a time constant of 15 ms. 

Calculate the charge stored in the capacitor after 12 ms.

3b3 marks
(i)

Sketch the current-time graph for a charging capacitor

(ii)

For a given potential difference, V, explain how you could find the energy stored in the capacitor at any given time from the graph.

3c3 marks

The graph in Figure 1 shows how the potential difference (p.d.) V varies with the charge Q stored by a different capacitor as V is increased from 9.0 V to 12.0 V. 

Figure 1

7-7-s-q--q3c-medium-aqa-a-level-physics

Use Figure 1 to determine an accurate value for the capacitance of this capacitor.

3d4 marks

When the capacitor is discharged through a fixed resistor R, the charge decreases by 90% in 35 s. 

Calculate the resistance of R in kΩ.

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4a2 marks

Figure 1 shows a circuit consisting of a resistor and a capacitor of capacitance 7.1 µF. 

 Figure 1

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Switch begin mathsize 16px style S subscript 1 end style  is closed and switch begin mathsize 16px style S subscript 2 end style is left open. 

Calculate the charge stored by the capacitor.

4b3 marks

Switch begin mathsize 16px style S subscript 1 end style is now opened and switch S subscript 2 is closed. 

Describe and explain in terms of the movement of electrons how the potential difference across the capacitor changes.

4c2 marks

The time constant of the circuit when the capacitor is discharging is 5.0 minutes. 

Figure 2

7-7-s-q--q4c-medium-aqa-a-level-physics

Sketch a graph on Figure 2 to show how the potential across the fixed resistor varies with time for the first 12 minutes after switch S subscript 2 closes.

4d3 marks

Calculate the initial current in the circuit when the capacitor begins to discharge.

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5a2 marks

A 590 nF capacitor is charged fully from a 20 V battery. At time t = 0 the capacitor begins to discharge through a resistor. When t = 15 s the energy remaining in the capacitor is one eighth of the energy it stored at 20 V. 

Show that the potential difference across the capacitor when t = 15 s is around 7 V. 

5b3 marks

Calculate time constant of this circuit.

5c2 marks

Calculate the resistance of the fixed resistor in MΩ.

5d4 marks

A student decides to confirm the value of the capacitance of this capacitor by determining the time constant of the circuit when the capacitor discharges through a fixed resistor. 

Describe an experiment to do this. Include in your answer: 

  • A circuit diagram.
  • An outline of a procedure.
  • An explanation of how you would use the data to determine the time constant.

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1a4 marks

A signal generator is used to produce a square wave, which is an oscillating voltage between 0 V and some maximum. It is connected to an oscilloscope, and the waveform generated is shown in Figure 1. 

The Y-voltage gain is set to 2 V div–1 and the time-base is set to 0.5 ms. 

Figure 1

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The signal generator and oscilloscope are then connected to a capacitor C and resistor R, which has a resistance of 2.2 kΩ, as shown in Figure 2. 

Figure 2

TYb32Q1S_7-7-s-q--q1a-fig-2-hard-aqa-a-level-physics-png

Sketch the waveform shown by the oscilloscope over one complete period.

1b4 marks

Describe how the waveform displayed on the oscilloscope in Figure 1 could be used to determine the capacitance of the capacitor C. 

Where appropriate, include calculations in your response.

1c3 marks

Discuss how the settings on the oscilloscope could be adjusted to reduce the uncertainty in determining the time constant. 

1d4 marks

The circuit in Figure 2 is now adjusted by placing an identical resistor in parallel with R. This changes the waveform displayed by the oscilloscope. 

Discuss the effects on the circuit and on the shape of the waveform displayed on the capacitor following the adjustment made to the circuit. You may wish to include a sketch with your answer.

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2a5 marks

Free falling bodies can be used to measure the gravitational field strength, g. Typically, this requires measurements of distance and time. 

A lab technician wants to determine if more accurate measurements of g can be achieved by using a capacitor instead of a stopwatch. She invents a setup using a steel ball bearing, which is connected to a capacitor and power source using steel contacts. 

The capacitoris fully charged to a voltage V subscript 0 after which the ball bearing is released. As it falls, the capacitor discharges through a resistor, until the ball bearing collides with a trap door which breaks the circuit. The voltage across the capacitor at this instant is V.  

Figure 1 and Figure 2 show a front and side view of the setup. 

 

    Figure 1: front view                                                Figure 2: side view

7-7-s-q--q2a-hard-aqa-a-level-physics

Show that the distance travelled by the ball bearing, s is given by: 

         s = 8g (lnbegin mathsize 16px style open parentheses V subscript 0 over V close parentheses end style)2

2b6 marks

Suggest how the lab technician should carry out the experiment to determine a value for g. 

Include reference to the independent and dependent variables, any data processing required, and how the data should be appropriately analysed.

2c4 marks

The technician tests the set up and is satisfied that all works as expected, with an initial voltage of 10.00 V and a final voltage of 8.74 V as the ball bearing collides with the trap door. 

She states that there is a smaller uncertainty in the value of g from this experimental method than the traditional way of measuring displacement s and time t directly using a stopwatch.

Discuss the conclusion of the technician by comparing the sources of uncertainty in both experimental methods.

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3a3 marks

Pacemakers are devices which are used to deliver short pulses of charge to a patient who is suffering from a cardiac arrest. 

Figure 1 shows a circuit  that is used in such a pacemaker. 

Figure 1

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The capacitor is initially uncharged when at t = 0 s, then the two-way switch connects it to a power supply of 4.0 kV. 

Sketch the graph on the axes provided in Figure 2 that shows how the voltage across the capacitor varies over 10 seconds. 

Figure 2

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3b3 marks

Show that the time taken for the charge stored in the capacitor to reach 5.0 mC is approximately 0.3 s.  

3c2 marks

Pacemaker manufacturers need efficient ways of measuring how quickly the charge and energy are released by capacitors. 

One approach uses the ‘exponential factor’ σ, which is a ratio of the energy remaining in a capacitor E to its initial energy stored E subscript 0 . For a given time interval, a smaller ratio indicates a quicker greater discharge of energy. 

Show that the exponential factor σ is given by:

            σ = begin mathsize 20px style e to the power of negative fraction numerator 2 t over denominator R C end fraction end exponent end style

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4a4 marks

A student sets up an experiment to investigate energy transfers between a projectile and a capacitor. 

They arrange the apparatus so that, if they flick a ball bearing of mass m = 40 g from the top of a bench, it collides with the centre of two pieces of metal foil which are 0.50 m apart and connected in an electric circuit as shown in Figure 1. 

As the ball bearing collides with the first metal strip, the capacitor begins to discharge through the resistor. As the ball bearing collides with the second metal strip, the capacitor stops discharging.  

Figure 1

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The results of the experiment are shown in Table 1: 

Table 1

 

Initial voltage / V

Final voltage / V

Trial 1

2.0

1.1

Trial 2

2.0

0.9

Trial 3

2.0

1.0

 

Using the information given in Figure 1 and Table 1, calculate the horizontal speed of the ball bearing.

4b4 marks

As the ball is struck, you may assume the vertical descent between the bench and the first metal strip is negligible. 

Show that the ball bearing transfers approximately 100 times more potential energy than the capacitor in the time taken for it to discharge.

4c3 marks

The capacitor in Figure 1 is replaced with an unmarked capacitor, and the experiment is repeated for one additional trial.

 The results of this trial are included in Table 2: 

Table 2

 

Initial voltage / V

Final voltage / V

Trial 1

2.0

1.1

Trial 2

2.0

0.9

Trial 3

2.0

1.0

Trial 4

2.0

0.2

Use the data in Table 2 to determine the capacitance of the unmarked capacitor and comment on whether your answer is as expected.

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