AP Physics 2 : Capacitors and Electric Fields

Study concepts, example questions & explanations for AP Physics 2

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Example Questions

Example Question #1 : Capacitors And Electric Fields

\(\displaystyle 3.0\: \mu F\) parallel-plate capacitor is connected to a constant voltage source. If the distance between the plates of this capacitor is \(\displaystyle 4\:mm\) and the capacitor holds a charge of \(\displaystyle 12.0\: \mu C\), what is the value of the electric field between the plates of this capacitor?

Possible Answers:

\(\displaystyle 1\frac{V}{m}\)

\(\displaystyle 10\frac{V}{m}\)

\(\displaystyle 1000\frac{V}{m}\)

An electric field does not exist between the plates of a parallel-plate capacitor

\(\displaystyle 100\frac{V}{m}\)

Correct answer:

\(\displaystyle 1000\frac{V}{m}\)

Explanation:

To solve this problem, we first need to solve for the voltage across the capacitor. For this, we'll need the formula for capacitance:

\(\displaystyle C=\frac{Q}{V}\)

Solving for the voltage:

\(\displaystyle V=\frac{Q}{C}=\frac{12.0\cdot 10^{-6}C}{3.0\cdot 10^{-6}F}=4.0V\)

Now that we have the voltage, we can make use of the following equation to solve for the electric field:

\(\displaystyle V=Ed\)

\(\displaystyle E=\frac{V}{d}=\frac{4.0V}{4\cdot 10^{-3}m}=1000\frac{V}{m}\)

Example Question #2 : Capacitors And Electric Fields

A set of parallel plate capacitors with a surface area of \(\displaystyle 12m^2\) has a total amount of charge equal to \(\displaystyle 4C\). What is the electric field between the plates?

\(\displaystyle \epsilon=8.85\cdot 10^{-12}\frac{F}{m}\)

Possible Answers:

\(\displaystyle 5.34\cdot 10^{10}\frac{N}{C}\)

\(\displaystyle 8.54\cdot 10^{9}\frac{N}{C}\)

\(\displaystyle 6.67\cdot 10^{9}\frac{N}{C}\)

\(\displaystyle 8.12\cdot 10^{10}\frac{N}{C}\)

\(\displaystyle 3.77\cdot 10^{10}\frac{N}{C}\)

Correct answer:

\(\displaystyle 3.77\cdot 10^{10}\frac{N}{C}\)

Explanation:

The equation for the electric field between two parallel plate capacitors is:

\(\displaystyle E=\frac{\sigma}{\epsilon}\)

Sigma is the charge density of the plates, which is equal to:

\(\displaystyle \sigma = \frac{Q}{A}\)

We are given the area and total charge, so we use them to find the charge density.

\(\displaystyle \sigma&=\frac{4}{12}\)

\(\displaystyle \sigma= 0.3334\frac{C}{m^2}\)

Now that we have the charge density, divide it by the vacuum permittivity to find the electric field.

\(\displaystyle E=\frac{0.3334}{8.85\times10^{-12}}=3.77\times10^{10}\frac{N}{C}\)

Example Question #3 : Capacitors And Electric Fields

Imagine a capacitor with a magnitude of charge Q on either plate. This capacitor has area A, separation distance D, and is not connected to a battery of voltage V. If some external agent pulls the capacitor apart such that D doubles, did the electric field, E, stored in the capacitor increase, decrease or stay the same?

Possible Answers:

Decreases

Stays constant

We need to know

Increases

Correct answer:

Stays constant

Explanation:

Relevant equations:

\(\displaystyle C=\frac{\varepsilon_{o}A}{D}\)

\(\displaystyle Q=CV\)

 \(\displaystyle U=\frac{1}{2}\frac{Q^{2}}{C}\)

Considering we are dealing with regions of charge instead of a point charge (or a charge that is at least spherical symmetric), it would be wise to consider using the definition of the electric field here:

\(\displaystyle E=\frac{V}{D}\)

We are only considering magnitude so the direction of the electric field is not of concern. Considering a battery is not connected, we can't claim the V is constant. So we use the second equation to substitute for V in the above equation:

\(\displaystyle E=\frac{Q}{CD}\)

Substitute C from the first equation:

\(\displaystyle E=\frac{Q\varepsilon _{o}D}{AD}\)

We see here that D actually cancels. This would not have been obvious without the previous substitution. Final result:

\(\displaystyle E=\frac{\varepsilon _{o}Q}{A}\)

These 3 quantities are static in this situation so E does not change.

Example Question #2 : Capacitors And Electric Fields

Imagine a capacitor with a magnitude of charge Q on either plate. This capacitor has area A, separation distance D, and is connected to a battery of voltage V. If some external agent pulls the capacitor apart such that D doubles, did the electric field, E, stored in the capacitor increase, decrease or stay the same?

Possible Answers:

Stays constant

Decreases by exactly \(\displaystyle \frac{1}{4}\)

Increases by exactly \(\displaystyle \frac{1}{2}\)

Decreases by exactly \(\displaystyle \frac{1}{2}\)

Correct answer:

Decreases by exactly \(\displaystyle \frac{1}{2}\)

Explanation:

Relevant equations:

\(\displaystyle C=\frac{\varepsilon_{o}A}{D}\)

\(\displaystyle Q=CV\)

 \(\displaystyle U=\frac{1}{2}\frac{Q^{2}}{C}\)

Considering we are dealing with regions of charge instead of a point charge (or a charge that is at least spherical symmetric), it would be wise to consider using the definition of the electric field here:

\(\displaystyle E=\frac{V}{D}\)

The battery maintains a constant V so we can directly relate E and D. Since D is doubled, E will be halved. 

Example Question #3 : Capacitors And Electric Fields

Lazy capacitor

If \(\displaystyle V_1=24V\), each plate of the capacitor has surface area \(\displaystyle 240 cm^2\), and the plates are \(\displaystyle .5mm\) apart, determine the electric field between the plates.

Possible Answers:

\(\displaystyle 1.6*10^4 \frac{N}{C}\)

\(\displaystyle 4.8*10^4 \frac{N}{C}\)

\(\displaystyle 4.0*10^4 \frac{N}{C}\)

\(\displaystyle 5.5*10^4 \frac{N}{C}\)

\(\displaystyle 6.6*10^4 \frac{N}{C}\)

Correct answer:

\(\displaystyle 4.8*10^4 \frac{N}{C}\)

Explanation:

The voltage rise through the source must be the same as the drop through the capacitor.

\(\displaystyle V_1=V_{C1}\)

The voltage drop across the capacitor is the equal to the electric field multiplied by the distance.

\(\displaystyle V_{C1}=E*d\)

Combine these equations and solve for the electric field:

\(\displaystyle V_1=E*d\)

\(\displaystyle \frac{V_1}{d}=E\)

Convert mm to m and plug in values:

\(\displaystyle \frac{24}{.0005}=E\)

\(\displaystyle E=4.8*10^4 \frac{N}{C}\)

Example Question #4 : Capacitors And Electric Fields

Lazy capacitor

If \(\displaystyle V_1=60V\), each plate of the capacitor has surface area \(\displaystyle 600 cm^2\), and the plates are \(\displaystyle 1mm\) apart, determine the excess charge on the positive plate.

Possible Answers:

\(\displaystyle 50.6nC\)

\(\displaystyle 31.9nC\)

\(\displaystyle 25.4nC\)

\(\displaystyle 48.8nC\)

\(\displaystyle 27.7nC\)

Correct answer:

\(\displaystyle 31.9nC\)

Explanation:

The voltage rise through the source must be the same as the drop through the capacitor.

\(\displaystyle V_1=V_{C1}\)

The voltage drop across the capacitor is the equal to the electric field multiplied by the distance.

\(\displaystyle V_{C1}=E*d\)

Combine equations and solve for the electric field:

\(\displaystyle V_1=E*d\)

\(\displaystyle \frac{V_1}{d}=E\)

Convert mm to m and plugging in values:

\(\displaystyle \frac{60V}{.001}=E\)

\(\displaystyle 60000\frac{N}{C}=E\)

Use the electric field in a capacitor equation:

\(\displaystyle E=\frac{q}{A*\epsilon_0}\)

Combine equations:

\(\displaystyle E*\epsilon_0*A=q\)

Converting \(\displaystyle cm^2\) to \(\displaystyle m^2\) and plug in values:

\(\displaystyle 60000*8.85*10^{-12}*.06=q\)

\(\displaystyle 31.9nC=q\)

Example Question #5 : Capacitors And Electric Fields

Lazy capacitor

Consider the given diagram. If \(\displaystyle V_1=4V\), each plate of the capacitor has surface area \(\displaystyle 100 cm^2\), and the plates at \(\displaystyle 1mm\) apart, determine the electric field between the plates.

Possible Answers:

\(\displaystyle 2000\frac{N}{C}=E\)

\(\displaystyle 7000\frac{N}{C}=E\)

\(\displaystyle 9000\frac{N}{C}=E\)

\(\displaystyle 3333\frac{N}{C}=E\)

\(\displaystyle 4000\frac{N}{C}=E\)

Correct answer:

\(\displaystyle 4000\frac{N}{C}=E\)

Explanation:

The voltage rise through the source must be the same as the drop through the capacitor.

\(\displaystyle V_1=V_{C1}\)

The voltage drop across the capacitor is the equal to the electric field multiplied by the distance.

\(\displaystyle V_{C1}=E*d\)

Combine equations and solve for the electric field:

\(\displaystyle V_1=E*d\)

\(\displaystyle \frac{V_1}{d}=E\)

Convert mm to m and plug in values:

\(\displaystyle \frac{V_1}{d}=E\)

\(\displaystyle 4000\frac{N}{C}=E\)

Example Question #1 : Capacitors And Electric Fields

Lazy capacitor

In the given circuit, the capacitor is made of two parallel circular plates of radius \(\displaystyle .3cm\) that are \(\displaystyle 2.5mm\) apart. If \(\displaystyle V_1\) is equal to \(\displaystyle 5V\), determine the electric field between the plates.

Possible Answers:

None of these

\(\displaystyle 1500\frac{N}{C}\)

\(\displaystyle 2000\frac{N}{C}\)

\(\displaystyle 2500\frac{N}{C}\)

\(\displaystyle 200\frac{N}{C}\)

Correct answer:

\(\displaystyle 2000\frac{N}{C}\)

Explanation:

Since it is the only element in the circuit besides the source, the voltage drop across the capacitor must be equal to the voltage gain in the capacitor.

\(\displaystyle V_1=V_{C1}\)

Definition of voltage:

\(\displaystyle V=E*d\)

Combine equations:

\(\displaystyle V_1=E_{C1}*d\)

Solve for \(\displaystyle E_{C1}\)

\(\displaystyle \frac{V}{d}=E_{C1}\)

Convert to meters and plug in values:

\(\displaystyle \frac{5}{.0025}=E_{C1}\)

\(\displaystyle 2000\frac{N}{C}=E_{C1}\)

Example Question #7 : Capacitors And Electric Fields

A parallel plate capacitor with a separation of \(\displaystyle .5\textup{ mm}\) and surface area \(\displaystyle 150\textup{ cm}^2\) is in series with a \(\displaystyle 9\textup{ V}\) battery. How will the electric field in the capacitor change if the separation is doubled?

Possible Answers:

Halved

It will stay the same

Tripled

Quadrupled

Doubled

Correct answer:

Halved

Explanation:

The voltage drop through the capacitor needs to be equal to the voltage of the battery.

\(\displaystyle V_b=V_c\)

The voltage drop of a parallel plate capacitor is equal to the internal electric field times the distance between them.

\(\displaystyle V_c=E*d\)

Combing equations and solving for \(\displaystyle E\)

\(\displaystyle E=\frac{V_b}{d}\)

From this, it can be seen that doubling the separation will halve the electric field.

Example Question #1 : Capacitors And Electric Fields

A parallel plate capacitor with a separation of \(\displaystyle .5\textup{ mm}\) and surface area \(\displaystyle 150\textup{ cm}^2\) is in series with a \(\displaystyle 9\textup{ V}\) battery. How will the electric field in the capacitor change if a second \(\displaystyle 9 \textup{ V}\) battery is added in series?

Possible Answers:

Impossible to determine

No change

Tripled

Doubled

Halved

Correct answer:

Doubled

Explanation:

The voltage drop through the capacitor needs to be equal to the voltage of the battery.

\(\displaystyle V_b=V_c\)

The voltage drop of a parallel plate capacitor is equal to the internal electric field times the distance between them.

\(\displaystyle V_c=E*d\)

Combing equations and solving for \(\displaystyle E\)

\(\displaystyle E=\frac{V_b}{d}\)

From this, it can be seen that doubling the voltage of the battery will doubled the electric field inside the capacitor.

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