AP Physics C- E&M- 8.5 Electric Flux - Exam Style questions - FRQs- New Syllabus

Question

A nonconducting rod of uniform positive linear charge density is near a sphere with charge \(-2.0\,\text{nC}\). The rod and sphere are held at rest on the \(x\)-axis, as shown in Figure \(1\). Equipotential lines and positions \(A\), \(B\), \(C\), \(D\), and \(E\) are labeled. Adjacent tick marks on the \(x\)-axis and the \(y\)-axis are \(0.40\,\text{m}\) apart.
 
(a) Calculate the absolute value of the electric flux through the Gaussian surface whose cross section is the \(-20.0\,\text{V}\) equipotential line.
A positive test charge is placed and held at rest at Position \(C\). An external force is applied to the test charge to move the test charge to different positions in the order of \(C \to E \to D \to A\). The test charge is momentarily at rest at each position.
(b) The bar shown in Figure \(2\) represents the absolute value of the work \(W_{CE}\) done by the external force on the test charge to move the test charge from Position \(C\) to Position \(E\).
i. Complete the following tasks for Figure \(2\).
• Draw a bar to represent the relative absolute value of the work \(W_{ED}\) done by the external force on the charge to move the test charge from Position \(E\) to Position \(D\).
• Draw a bar to represent the relative absolute value of the work \(W_{DA}\) done by the external force on the charge to move the test charge from Position \(D\) to Position \(A\).
• The height of each bar should be proportional to the value of \(W_{CE}\). If \(W_{ED}=0\) and/or \(W_{DA}=0\), write a \(0\) in the corresponding column, as appropriate.
ii. Calculate the approximate magnitude of the \(x\)-component of the electric field at Position \(B\).
The positive test charge is placed at Position \(D\). The test charge is then released from rest.
(c) Indicate the direction, not components, of the net electric force exerted on the test charge immediately after the charge is released from rest.
_____ \(+x\)      _____ \(+y\)      _____ Directly away from the sphere
_____ \(-x\)      _____ \(-y\)      _____ Directly toward the sphere
Without using equations, justify your answer using physics principles.
The sphere and the test charge are removed. A rod has length \(4L\) and uniform positive linear charge density \(+\lambda\). The rod is held at rest on the \(x\)-axis and is positioned as shown in Figure \(3\). Position \(P\), not shown, is located on the \(x\)-axis a distance \(x_P\) from the origin, where \(x_P>4L\).
(d) The electric potential \(V_P\) at \(x_P\) is
\(V_P=k\lambda\ln\left|\dfrac{x_P}{x_P-4L}\right|\)
i. Using integral calculus, derive the expression for \(V_P\) provided.
ii. On Figure \(4\), sketch a graph of the \(x\)-component \(E_x\) of the electric field from the rod as a function of \(x\) in the region \(4L<x<12L\).
 

Most-appropriate topic codes (AP Physics C: Electricity and Magnetism):

• Topic \(8.4\) — Electric Fields of Charge Distributions (Part \( \mathrm{d} \))
• Topic \(8.5\) — Electric Flux (Part \( \mathrm{a} \))
• Topic \(8.6\) — Gauss’s Law (Part \( \mathrm{a} \))
• Topic \(9.2\) — Electric Potential (Parts \( \mathrm{b} \), \( \mathrm{c} \), \( \mathrm{d} \))
▶️ Answer/Explanation

(a)
Use Gauss’s law:

\(\Phi_E=\dfrac{Q_{\text{enc}}}{\varepsilon_0}\)

The \(-20.0\,\text{V}\) equipotential line encloses the charged sphere. The charge enclosed is

\(Q_{\text{enc}}=-2.0\times10^{-9}\,\text{C}\)

The problem asks for the absolute value of the flux:

\( |\Phi_E| = \left|\dfrac{-2.0\times10^{-9}}{8.85\times10^{-12}}\right| \)

\( |\Phi_E|=2.26\times10^{2}\,\text{N}\cdot\text{m}^2/\text{C} \)

\( \boxed{|\Phi_E|=226\,\text{N}\cdot\text{m}^2/\text{C}} \)

(b)(i)
For a positive test charge moved slowly from one equipotential to another, the work done by the external force is proportional to the absolute value of the change in electric potential:

\( |W_{\text{ext}}|=q|\Delta V| \)

Since \(D\) and \(E\) are on the same equipotential line,

\( W_{ED}=0 \)

Therefore, the \(W_{ED}\) column should have a \(0\).

The work from \(D\) to \(A\) corresponds to a larger potential difference than the work from \(C\) to \(E\). Since the given \(W_{CE}\) bar is \(4\) units tall, the \(W_{DA}\) bar should be \(6\) units tall.

\( \boxed{W_{ED}=0} \)

\( \boxed{W_{DA}\text{ should be }6\text{ units tall}} \)

(b)(ii)
The electric field component is related to electric potential by

\( E_x=-\dfrac{dV}{dx} \)

An approximate magnitude can be found from nearby equipotential lines:

\( |E_x|\approx \left|\dfrac{\Delta V}{\Delta x}\right| \)

Near Position \(B\), the potential changes from about \(20.0\,\text{V}\) to \(0.0\,\text{V}\) over about \(0.65\,\text{m}\).

\( |E_x|\approx \left|\dfrac{20.0\,\text{V}-0.0\,\text{V}}{0.65\,\text{m}}\right| \)

\( |E_x|\approx 31\,\text{V/m} \)

\( \boxed{|E_x|\approx 31\,\text{V/m}} \)

(c)
Correct direction:

\( \boxed{+y} \)

The electric field is perpendicular to the equipotential line at Position \(D\). A positive test charge experiences an electric force in the same direction as the electric field. Since a positive charge moves from higher electric potential to lower electric potential when released, the force at \(D\) is directed upward, or in the \(+y\)-direction.

(d)(i)
The electric potential due to a small charge element is

\( dV=\dfrac{k\,dq}{r} \)

For the uniformly charged rod,

\( dq=\lambda\,dx \)

A charge element at position \(x\) is a distance

\( r=x_P-x \)

from point \(P\). Therefore,

\( dV=\dfrac{k\lambda\,dx}{x_P-x} \)

The rod extends from \(x=0\) to \(x=4L\), so

\( V_P=\int_0^{4L}\dfrac{k\lambda}{x_P-x}\,dx \)

Factor out the constants:

\( V_P=k\lambda\int_0^{4L}\dfrac{1}{x_P-x}\,dx \)

Since

\( \int \dfrac{1}{x_P-x}\,dx=-\ln|x_P-x| \)

then

\( V_P=k\lambda\left[-\ln|x_P-x|\right]_0^{4L} \)

\( V_P=k\lambda\left[-\ln|x_P-4L|+\ln|x_P|\right] \)

\( V_P=k\lambda\ln\left|\dfrac{x_P}{x_P-4L}\right| \)

\( \boxed{V_P=k\lambda\ln\left|\dfrac{x_P}{x_P-4L}\right|} \)

(d)(ii)
For \(4L<x<12L\), the electric field points in the \(+x\)-direction because the rod is positively charged and the point is to the right of the rod.

The field is strongest just to the right of \(x=4L\), then decreases as \(x\) increases. The graph should therefore be:

• always positive for \(4L<x<12L\)
• very large near \(x=4L\)
• decreasing as \(x\) increases
• concave up, approaching \(0\) as \(x\) gets far from the rod

A consistent expression for the field is

\( E_x=-\dfrac{dV}{dx} \)

or directly from the rod,

\( E_x=k\lambda\left(\dfrac{1}{x-4L}-\dfrac{1}{x}\right) \)

\( E_x=\dfrac{4k\lambda L}{x(x-4L)} \)

This expression is positive and decreases as \(x\) increases, matching the required sketch.

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