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AP Physics 2- 12.1 Magnetic Fields- Exam Style questions - FRQs- New Syllabus

Magnetic Fields AP  Physics 2 FRQ

Unit 12: Magnetism and Electromagnetic Induction

Weightage : 15–18%

AP Physics 2 Exam Style Questions – All Topics

Question

At the instant shown above, a negatively charged object is moving to the left with constant velocity \(v\) near a long, straight wire that has a current \(I\) directed to the left. The region contains a uniform electric field of magnitude \(E\), and the charged object is at a distance \(d\) from the wire. The figure shows the electric and magnetic forces, \(F_E\) and \(F_M\), respectively, exerted on the charged object.
(a) Derive an expression for \(v\) in terms of \(E\), \(d\), \(I\), and physical constants, as appropriate.
(b) The charged object is removed, and a square coil with side length \(2L\) is placed near the long, straight wire, as shown above. The bottom of the coil is a distance \(L\) from the wire. The magnitude of the magnetic field due to the current in the wire is \(3B_0\) at point \(P_1\) and \(B_0\) at point \(P_2\).
i. Write an “\(X\)” at a location on the figure where the magnitude of the magnetic field is \(2B_0\). Briefly justify your reasoning.
ii. Over a time interval of \(2.0\,\text{s}\), the current in the wire is decreased. The initial magnetic flux through the coil is \(5.0\times 10^{-5}\,\text{T}\cdot\text{m}^2\), and the final magnetic flux through the coil is \(1.0\times 10^{-5}\,\text{T}\cdot\text{m}^2\). The coil has a total resistance of \(10\,\Omega\). Calculate the magnitude of the average current in the coil during the \(2.0\,\text{s}\) time interval.
The wire is removed and the square coil is positioned so that the coil is directly above and concentric with a round coil of wire connected to a power supply. A part of the square coil is removed and a lightbulb is connected to the coil, as shown above.
(c) During a short time interval, the current in the power supply is constantly increasing. Use physics principles to explain why the lightbulb is lit during the entire time interval.

Most-appropriate topic codes (AP Physics 2):

• Topic \(12.1\) — Magnetic Fields (Part \( \mathrm{(a)} \), Part \( \mathrm{(b)} \), Part \( \mathrm{(c)} \))
• Topic \(12.2\) — Magnetism and Moving Charges (Part \( \mathrm{(a)} \))
• Topic \(12.3\) — Magnetism and Current-Carrying Wires (Part \( \mathrm{(a)} \), Part \( \mathrm{(b)} \))
• Topic \(12.4\) — Electromagnetic Induction and Faraday’s Law (Part \( \mathrm{(b)(ii)} \), Part \( \mathrm{(c)} \))
▶️ Answer/Explanation

(a)
Since the charged object moves with constant velocity, the net force on the object is \(0\). Therefore, the magnetic force and electric force must have equal magnitudes.

\(F_M=F_E\)

The electric force on the charged object has magnitude \(F_E=qE\), where \(q\) is the magnitude of the charge.

The magnetic force on the moving charged object has magnitude \(F_M=qvB\), because the velocity is perpendicular to the magnetic field at the location of the object.

Set the magnitudes equal:

\(qvB=qE\)

Cancel \(q\):

\(vB=E\)

The magnetic field a distance \(d\) from a long, straight current-carrying wire is

\(B=\dfrac{\mu_0 I}{2\pi d}\)

Substitute this expression into \(vB=E\):

\(v\left(\dfrac{\mu_0 I}{2\pi d}\right)=E\)

Solve for \(v\):

\(\boxed{v=\dfrac{2\pi dE}{\mu_0 I}}\)

The charge \(q\) cancels because both the electric and magnetic forces are proportional to the charge magnitude.

(b)(i)
The “\(X\)” should be placed between point \(P_1\) and the dashed horizontal line through the middle of the coil.

The magnetic field due to a long, straight wire is inversely proportional to the distance from the wire:

\(B=\dfrac{\mu_0 I}{2\pi r}\)

Since \(B\propto \dfrac{1}{r}\), the magnetic field is stronger closer to the wire and weaker farther from the wire.

At point \(P_1\), the magnetic field is \(3B_0\). At point \(P_2\), the magnetic field is \(B_0\). A field of \(2B_0\) is between these values, so the point must be somewhere between \(P_1\) and \(P_2\).

More specifically, because \(P_1\) is closer to the wire and \(2B_0\) is less than \(3B_0\), the \(X\) must be above \(P_1\). Because \(2B_0\) is still greater than \(B_0\), it must be below \(P_2\). The correct location is between \(P_1\) and the dashed line.

(b)(ii)
Use Faraday’s law to find the magnitude of the induced emf:

\(|\varepsilon|=\left|\dfrac{\Delta \Phi_B}{\Delta t}\right|\)

The change in magnetic flux is

\(\Delta \Phi_B=\Phi_{B,f}-\Phi_{B,i}\)

\(\Delta \Phi_B=\left(1.0\times 10^{-5}\,\text{T}\cdot\text{m}^2\right)-\left(5.0\times 10^{-5}\,\text{T}\cdot\text{m}^2\right)\)

\(\Delta \Phi_B=-4.0\times 10^{-5}\,\text{T}\cdot\text{m}^2\)

The magnitude is

\(|\Delta \Phi_B|=4.0\times 10^{-5}\,\text{T}\cdot\text{m}^2\)

So the magnitude of the induced emf is

\(|\varepsilon|=\dfrac{4.0\times 10^{-5}\,\text{T}\cdot\text{m}^2}{2.0\,\text{s}}\)

\(|\varepsilon|=2.0\times 10^{-5}\,\text{V}\)

Now use Ohm’s law:

\(I_{\text{coil}}=\dfrac{|\varepsilon|}{R}\)

\(I_{\text{coil}}=\dfrac{2.0\times 10^{-5}\,\text{V}}{10\,\Omega}\)

\(\boxed{I_{\text{coil}}=2.0\times 10^{-6}\,\text{A}}\)

The average current is very small, but it is nonzero because the magnetic flux through the coil is changing.

(c)
The current in the round coil produces a magnetic field around the round coil.

Since the square coil is placed above and concentric with the round coil, some of the magnetic field from the round coil passes through the area enclosed by the square coil. This produces magnetic flux through the square coil.

During the time interval, the current in the power supply is constantly increasing. Since the current in the round coil increases, the magnetic field produced by the round coil also increases.

Because the magnetic field through the square coil changes, the magnetic flux through the square coil changes.

By Faraday’s law, a changing magnetic flux induces an emf:

\(|\varepsilon|=\left|\dfrac{\Delta \Phi_B}{\Delta t}\right|\)

The induced emf causes an induced current in the square coil circuit. Since the lightbulb is connected in that circuit, the induced current passes through the lightbulb.

Therefore, the lightbulb remains lit during the entire time interval because the current in the round coil is changing during the entire time interval, so the magnetic flux through the square coil is also changing during the entire time interval.

\(\boxed{\text{Changing current } \rightarrow \text{ changing magnetic field } \rightarrow \text{ changing flux } \rightarrow \text{ induced current in the bulb.}}\)

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