Magnetism and Moving Charges

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AP Physics C: Electricity and Magnetism › Magnetism and Moving Charges

Questions 1 - 10
1

In a lab, a straight wire carries $I=8.0,\text{A}$ upward. Moving charges in the wire create circular magnetic field lines around the wire; use the right-hand rule (thumb along current, curled fingers give $\vec B$ direction). A point $r=0.040,\text{m}$ east of the wire lies in air ($\mu_0=4\pi\times10^{-7},\text{T·m/A}$). Refer to the scenario above. Calculate the magnetic field strength at that point.

$1.0\times10^{-5},\text{T}$

$4.0\times10^{-5},\text{T}$

$8.0\times10^{-5},\text{T}$

$4.0\times10^{-5},\text{m/s}$

$2.0\times10^{-5},\text{T}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. The magnetic field around a straight current-carrying wire is given by B = μ₀I/(2πr), where the field forms concentric circles around the wire with direction determined by the right-hand rule. In this scenario, a wire carries 8.0 A upward, and we need to find the field strength at a point 0.040 m east of the wire. Choice E is correct because B = (4π×10⁻⁷)(8.0)/(2π×0.040) = 32×10⁻⁷/0.080 = 4.0×10⁻⁵/2 = 2.0×10⁻⁵ T. Choice A is incorrect as it represents double the correct value, likely from forgetting the factor of 2π in the denominator. To help students: emphasize the formula B = μ₀I/(2πr) for straight wires, practice unit analysis to ensure dimensional consistency, and use the right-hand rule to determine field direction (thumb along current, fingers curl in field direction).

2

A proton ($q=+e$, $m=1.67\times10^{-27},\text{kg}$) enters a uniform magnetic field $B=0.30,\text{T}$ with velocity perpendicular to $\vec B$. Moving charges create magnetic fields, but here the external field causes a Lorentz force $F=qvB$ that bends the path without changing speed. The proton speed is $v=2.4\times10^{6},\text{m/s}$. Refer to the scenario above. Explain why the charged particle follows a circular path in the magnetic field.

The force is zero because magnetic fields only affect stationary charges

The magnetic field does positive work each cycle to keep the circle closed

The particle curves because electric attraction to the magnet provides centripetal force

The force is parallel to velocity, so the particle spirals outward faster

The force is always perpendicular to velocity, acting as centripetal force

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. The magnetic force F = qvB acts perpendicular to both velocity and magnetic field, providing centripetal force for circular motion when v⊥B. In this scenario, a proton enters a magnetic field with velocity perpendicular to B, creating conditions for uniform circular motion. Choice A is correct because the Lorentz force is always perpendicular to velocity (from the cross product v×B), providing the centripetal force mv²/r = qvB needed for circular motion at constant speed. Choice D is incorrect because magnetic forces do no work (W = F·d = 0 when F⊥v), so energy cannot be transferred to maintain the motion. To help students: use vector diagrams showing F, v, and B at multiple points on the circle, emphasize the work-energy theorem showing magnetic forces do no work, and practice setting centripetal force equal to magnetic force.

3

A long straight wire carries $I=12,\text{A}$ to the right. Moving charges in the wire generate a magnetic field circling the wire; apply the right-hand rule to set $\vec B$ direction. A point is located $r=0.060,\text{m}$ above the wire in air. Refer to the scenario above. Calculate the magnetic field strength at that point.

$4.0\times10^{-5},\text{T}$

$4.0\times10^{-5},\text{N}$

$2.0\times10^{-5},\text{T}$

$1.3\times10^{-5},\text{T}$

$8.0\times10^{-5},\text{T}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. A straight current-carrying wire creates a magnetic field with magnitude B = μ₀I/(2πr) at distance r, forming concentric circles around the wire. In this scenario, a wire carries 12 A to the right, and we calculate the field 0.060 m above it. Choice B is correct because B = (4π×10⁻⁷)(12)/(2π×0.060) = 48π×10⁻⁷/(0.12π) = 48×10⁻⁷/0.12 = 4.0×10⁻⁵/2 = 2.0×10⁻⁵ T. Choice A represents double the correct value, a common error from omitting the 2π factor in the denominator. To help students: memorize B = μ₀I/(2πr) for straight wires, practice dimensional analysis to catch formula errors, and use the right-hand rule to find field direction (thumb along current, fingers curl in B direction).

4

A positive particle ($q=+2.0\times10^{-6},\text{C}$) moves at $v=1500,(\text{m/s})$ north through a uniform magnetic field $B=0.80,\text{T}$ directed east. Moving charges create magnetic fields, and the right-hand rule gives the direction of $\vec v\times\vec B$; the magnetic force magnitude is $F=qvB\sin\theta$. Refer to the scenario above. What is the direction of the magnetic force on a positive charge moving as described?

Upward

East

North

Downward

West

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. The magnetic force on a moving charge is F = qv×B, with direction found using the right-hand rule for the cross product, considering the charge sign. In this scenario, a positive charge moves north while the magnetic field points east, requiring careful application of the right-hand rule. Choice C is correct because using the right-hand rule: point fingers north (velocity), curl them east (field), and the thumb points downward (force direction for positive charge). Choice B would result from reversing the order of the cross product or misapplying the right-hand rule. To help students: practice the right-hand rule with orthogonal vectors, emphasize that v×B ≠ B×v (order matters), and use coordinate systems to verify directions (north×east = down in standard orientation).

5

A solenoid of length $0.30,\text{m}$ has $N=900$ turns and carries current $I=2.0,\text{A}$. The moving charges in the coils create a magnetic field; inside a long solenoid, $B\approx\mu_0 n I$ with $n=N/L$, and the right-hand rule (curl fingers with current, thumb gives $\vec B$ inside) sets direction. Refer to the scenario above. Calculate the magnetic field strength inside the solenoid.

$3.8\times10^{-3},\text{T}$

$2.4\times10^{-2},\text{T}$

$7.5\times10^{-3},\text{T}$

$7.5\times10^{-3},\text{m/s}$

$1.5\times10^{-2},\text{T}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. A solenoid creates a nearly uniform magnetic field inside with magnitude B = μ₀nI, where n = N/L is the turn density (turns per unit length). In this scenario, a solenoid has 900 turns over 0.30 m length carrying 2.0 A current. Choice A is correct because n = 900/0.30 = 3000 turns/m, so B = (4π×10⁻⁷)(3000)(2.0) = 24π×10⁻⁴ = 7.54×10⁻³ ≈ 7.5×10⁻³ T. Choice E represents double the correct value, possibly from using diameter instead of length or misapplying the formula. To help students: emphasize that n = N/L is turns per unit length, practice unit analysis to ensure consistency, and use the right-hand rule for solenoids (curl fingers with current, thumb points along B inside).

6

A wire segment of length $L=0.25,\text{m}$ carries $I=6.0,\text{A}$ upward through a uniform magnetic field $B=0.30,\text{T}$ directed to the right. Moving charges in the wire create magnetic fields, but the external field exerts a magnetic force on the current: $\vec F=I,\vec L\times\vec B$. Use the right-hand rule for $\vec L\times\vec B$. Refer to the scenario above. What is the direction of the magnetic force on a positive charge moving as described?

Out of the page

Upward

To the right

Into the page

Downward

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. A current-carrying wire in a magnetic field experiences force F = IL×B, where L points in the current direction and the cross product determines force direction. In this scenario, current flows upward (L upward) through a field pointing right, requiring the right-hand rule for L×B. Choice B is correct because using the right-hand rule: point fingers upward (current/L direction), curl them to the right (field), and the thumb points into the page (force direction). Choice D would result from confusing the cross product order or misapplying the right-hand rule. To help students: practice F = IL×B systematically, emphasize that L points along current flow, and verify directions using coordinate systems (up×right = into page in standard orientation).

7

A rectangular current loop (height $0.10,\text{m}$, width $0.060,\text{m}$) lies in a uniform magnetic field $B=0.40,\text{T}$ to the right. Current $I=3.0,\text{A}$ flows clockwise as viewed from above; moving charges in the wire create magnetic fields, and the loop experiences forces from the external field via $\vec F=I,\vec L\times\vec B$. The loop’s plane is vertical, so its area vector points north. Refer to the scenario above. Determine the net force on the loop in the given magnetic field.

Nonzero, into the page

Nonzero, upward

Nonzero, to the right

Zero, because $B$ is uniform only inside the loop

Zero, forces cancel pairwise

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. A current loop in a uniform magnetic field experiences forces on each segment given by F = IL×B, where the net force depends on the loop's orientation and field uniformity. In this scenario, a rectangular loop with clockwise current sits in a uniform field pointing right, with the loop's plane vertical. Choice C is correct because in a uniform field, the forces on opposite sides of the loop are equal in magnitude but opposite in direction, causing them to cancel pairwise - the top and bottom segments have opposing forces, as do the left and right segments. Choice A is incorrect because it ignores the cancellation of forces on opposite segments in a uniform field. To help students: draw force vectors on each segment using F = IL×B, show how opposite sides experience opposite forces, and emphasize that uniform fields produce zero net force but can create torque.

8

A positive ion ($q=+1.60\times10^{-19},\text{C}$) enters a uniform magnetic field $\vec B=0.50,\text{T}$ directed into the page. Its velocity is $v=2.0\times10^{6},\text{m/s}$ to the right, so moving charge produces no $\vec B$ here but feels Lorentz force $\vec F=q,\vec v\times\vec B$. Use the right-hand rule for $\vec v\times\vec B$. Refer to the scenario above. What is the direction of the magnetic force on a positive charge moving as described?

Upward

Downward

To the left

To the right

Into the page

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. The Lorentz force on a moving charge is F = qv×B, with direction determined by the right-hand rule for the cross product v×B, then considering the sign of the charge. In this scenario, a positive ion moves to the right while the magnetic field points into the page. Choice A is correct because using the right-hand rule: point fingers right (velocity), curl them into the page (field), and the thumb points upward (force direction for positive charge). Choice B would be correct for a negative charge, showing a common confusion about charge sign effects. To help students: practice the right-hand rule systematically - fingers along v, curl toward B, thumb shows F for positive charges; emphasize that negative charges experience force opposite to the right-hand rule result.

9

A long straight wire carries conventional current $I=12,\text{A}$ to the east. Moving charges in the wire create a magnetic field that forms concentric circles around the wire; use the right-hand rule (thumb along current, fingers give $\vec B$). At a point $r=3.0,\text{cm}$ directly above the wire, the field magnitude is $B=\mu_0 I/(2\pi r)$. Refer to the scenario above. Calculate the magnetic field strength at the point above the wire.

$8.0\times10^{-5},\text{m/s}$

$8.0\times10^{-5},\text{T}$

$2.4\times10^{-4},\text{T}$

$8.0\times10^{-4},\text{T}$

$8.0\times10^{-6},\text{T}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. The magnetic field around a straight current-carrying wire is given by B = μ₀I/(2πr), where μ₀ = 4π × 10⁻⁷ T·m/A. In this scenario, we need to calculate the field strength at r = 3.0 cm = 0.03 m from a wire carrying I = 12 A. Substituting values: B = (4π × 10⁻⁷)(12)/(2π × 0.03) = 8.0 × 10⁻⁵ T. Choice A is correct because it properly applies the formula with correct unit conversions and calculations. Choice B is incorrect because it represents an error of a factor of 10, likely from incorrect conversion of centimeters to meters or calculation error. To help students: Emphasize careful unit conversion (cm to m), practice using μ₀ = 4π × 10⁻⁷ T·m/A, and verify dimensions in the formula. Create a systematic approach: identify given values, convert units, substitute carefully, and check order of magnitude.

10

A solenoid (length $L=0.40,\text{m}$, $N=800$ turns) carries current $I=1.5,\text{A}$. The moving charges in its windings create a magnetic field that is approximately uniform inside and much weaker outside; the right-hand rule (fingers follow current, thumb gives $\vec B$ inside) sets direction. The field magnitude inside is $B\approx\mu_0 n I$ where $n=N/L$. Refer to the scenario above. Calculate the magnetic field strength inside the solenoid.

$3.8\times10^{-3},\text{N}$

$3.8\times10^{-2},\text{T}$

$3.8\times10^{-4},\text{T}$

$3.8\times10^{-3},\text{T}$

$1.9\times10^{-3},\text{T}$

Explanation

This question tests AP Physics C: Electricity and Magnetism skills, specifically understanding of magnetism and moving charges. The magnetic field inside a solenoid is approximately uniform and given by B = μ₀nI, where n = N/L is the turn density and μ₀ = 4π × 10⁻⁷ T·m/A. In this scenario, N = 800 turns, L = 0.40 m, so n = 800/0.40 = 2000 turns/m, and I = 1.5 A. Calculating: B = (4π × 10⁻⁷)(2000)(1.5) = 3.77 × 10⁻³ T ≈ 3.8 × 10⁻³ T. Choice A is correct because it properly calculates turn density and applies the solenoid field formula. Choice C is incorrect by a factor of 10, suggesting an error in calculating n or in the final multiplication. To help students: Emphasize that n is turns per unit length (not total turns), practice the solenoid formula B = μ₀nI, and verify units work out to Tesla. Draw solenoids showing how closely spaced turns create strong internal fields.

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