Magnetic Fields of Current-Carrying Wires

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AP Physics C: Electricity and Magnetism › Magnetic Fields of Current-Carrying Wires

Questions 1 - 8
1

A long, straight wire in vacuum carries $I=2.5,\text{A}$ upward. Point $P$ lies $d=0.015,\text{m}$ from the wire. Use $B=\dfrac{\mu_0 I}{2\pi d}$ with $\mu_0=4\pi\times10^{-7},\text{T·m/A}$. What is the magnitude of the magnetic field at point $P$ due to the wire?

$1.7\times10^{-5},\text{T}$

$3.3\times10^{-5},\text{T}$

$5.2\times10^{-4},\text{T}$

$3.3\times10^{-7},\text{T}$

Explanation

This question tests AP Physics C skills in applying the magnetic field formula for an infinite straight wire carrying current. The Biot-Savart Law for a long straight wire yields B = μ₀I/(2πd), where I is the current and d is the perpendicular distance from the wire. In this scenario, the wire carries I = 2.5 A upward, point P is at d = 0.015 m from the wire, and μ₀ = 4π × 10⁻⁷ T·m/A. Choice A is correct because it accurately calculates: B = (4π × 10⁻⁷ × 2.5)/(2π × 0.015) = (10π × 10⁻⁷)/(0.030π) = 3.33 × 10⁻⁵ T ≈ 3.3 × 10⁻⁵ T. Choice B is incorrect as it represents approximately half the correct value, suggesting a possible arithmetic error or extra factor of 2. To help students: emphasize careful cancellation of π terms, practice converting between different distance units, and verify answers using dimensional analysis. Drawing the wire with circular field lines helps students visualize that the field strength decreases with distance.

2

A long, straight wire in vacuum carries $I=12,\text{A}$ upward. Point $P$ lies $d=0.040,\text{m}$ from the wire. Use the Biot-Savart result for an infinite wire: $B=\dfrac{\mu_0 I}{2\pi d}$ with $\mu_0=4\pi\times10^{-7},\text{T·m/A}$. What is the magnitude of the magnetic field at point $P$ due to the wire?

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

$3.0\times10^{-5},\text{T}$

$6.0\times10^{-5},\text{T}$

$1.2\times10^{-4},\text{T}$

Explanation

This question tests AP Physics C skills in applying the Biot-Savart Law result for an infinite straight wire to calculate magnetic fields. For a long straight wire, the magnetic field at distance d is given by B = μ₀I/(2πd), where μ₀ is the permeability of free space. In this scenario, a current I = 12 A flows upward through the wire, and the field is calculated at point P located d = 0.040 m from the wire, with μ₀ = 4π × 10⁻⁷ T·m/A. Choice B is correct because it accurately applies the formula: B = (4π × 10⁻⁷ × 12)/(2π × 0.040) = (48π × 10⁻⁷)/(0.080π) = 6.0 × 10⁻⁵ T. Choice A is incorrect because it doubles the correct answer, likely from an error in the denominator calculation. To help students: emphasize canceling π terms carefully, practice unit analysis to verify T·m/A divided by m yields T, and encourage systematic substitution of values before simplifying. Drawing the wire configuration with field lines circling the wire helps visualize the geometry.

3

A circular loop of radius $R=0.080,\text{m}$ in free space carries $I=5.0,\text{A}$ clockwise. Use $B=\dfrac{\mu_0 I}{2R}$ at the loop center, with $\mu_0=4\pi\times10^{-7},\text{T·m/A}$. Calculate the magnetic field at the center of the loop.

$7.9\times10^{-5},\text{T}$

$7.9\times10^{-7},\text{T}$

$1.6\times10^{-4},\text{T}$

$3.9\times10^{-5},\text{T}$

Explanation

This question tests AP Physics C skills in calculating the magnetic field at the center of a circular current loop using the Biot-Savart Law result. For a circular loop of radius R carrying current I, the magnetic field at the center is B = μ₀I/(2R), where μ₀ is the permeability of free space. In this scenario, a current I = 5.0 A flows clockwise through a loop of radius R = 0.080 m, with μ₀ = 4π × 10⁻⁷ T·m/A provided. Choice A is correct because it properly applies the formula: B = (4π × 10⁻⁷ × 5.0)/(2 × 0.080) = (20π × 10⁻⁷)/0.16 = 3.9 × 10⁻⁵ T. Choice B is incorrect because it doubles the correct answer, suggesting an error in applying the factor of 2 in the denominator. To help students: stress that the formula already includes all geometric factors for the center point, practice careful arithmetic with scientific notation, and use the right-hand rule to determine field direction. Comparing this formula to the straight wire formula helps students see the different geometric factors.

4

A long, straight wire in vacuum carries $I=18,\text{A}$ upward. Point $P$ lies $d=0.12,\text{m}$ from the wire. Use $B=\dfrac{\mu_0 I}{2\pi d}$ with $\mu_0=4\pi\times10^{-7},\text{T·m/A}$. What is the magnitude of the magnetic field at point $P$ due to the wire?

$1.5\times10^{-5},\text{T}$

$9.4\times10^{-5},\text{T}$

$3.8\times10^{-6},\text{T}$

$3.0\times10^{-5},\text{T}$

Explanation

This question tests AP Physics C skills in applying the magnetic field formula for a long straight current-carrying wire derived from the Biot-Savart Law. The field at perpendicular distance d from an infinite wire with current I is B = μ₀I/(2πd), decreasing inversely with distance. In this scenario, the wire carries I = 18 A upward, point P is at d = 0.12 m, with μ₀ = 4π × 10⁻⁷ T·m/A. Choice A is correct because it accurately calculates: B = (4π × 10⁻⁷ × 18)/(2π × 0.12) = (72π × 10⁻⁷)/(0.24π) = 3.0 × 10⁻⁵ T. Choice B is incorrect as it represents half the correct value, possibly from an arithmetic error or extra factor of 2 in the denominator. To help students: practice systematic substitution before simplifying, emphasize that π cancels in this formula, and use dimensional analysis to verify units. Drawing field circles around the wire and marking the specific point P helps visualize the inverse distance relationship.

5

A circular loop of radius $R=0.12,\text{m}$ in free space carries $I=9.0,\text{A}$ clockwise. Use $B=\dfrac{\mu_0 I}{2R}$ at the loop center, with $\mu_0=4\pi\times10^{-7},\text{T·m/A}$. Calculate the magnetic field at the center of the loop.

$4.7\times10^{-5},\text{T}$

$1.2\times10^{-4},\text{T}$

$9.4\times10^{-6},\text{T}$

$4.7\times10^{-4},\text{T}$

Explanation

This question tests AP Physics C skills in calculating the magnetic field at the center of a circular current loop using the standard Biot-Savart result. For a loop of radius R with current I, the center field is B = μ₀I/(2R), with direction determined by the right-hand rule applied to the current direction. In this scenario, the loop has radius R = 0.12 m, carries I = 9.0 A clockwise, with μ₀ = 4π × 10⁻⁷ T·m/A. Choice B is correct because it properly applies: B = (4π × 10⁻⁷ × 9.0)/(2 × 0.12) = (36π × 10⁻⁷)/0.24 = 150π × 10⁻⁷ = 4.71 × 10⁻⁵ T ≈ 4.7 × 10⁻⁵ T. Choice A is incorrect as it represents about 2.5 times the correct value, suggesting a calculation error. To help students: emphasize careful arithmetic with decimals in scientific notation, practice problems with various loop sizes, and reinforce that the field is inversely proportional to radius. Comparing multiple loop configurations helps students recognize patterns in the field strength relationships.

6

A semi-circular arc of radius $R=0.20,\text{m}$ lies in a plane in free space. The arc carries uniform current $I=10,\text{A}$. Use $B=\dfrac{\mu_0 I}{4R}$ at the center, with $\mu_0=4\pi\times10^{-7},\text{T·m/A}$. Find the magnetic field at the center of the arc.

$3.1\times10^{-5},\text{T}$

$1.6\times10^{-5},\text{T}$

$6.3\times10^{-6},\text{T}$

$7.9\times10^{-6},\text{T}$

Explanation

This question tests AP Physics C skills in calculating the magnetic field at the center of a semicircular current-carrying arc using the Biot-Savart Law result. For a semicircular arc of radius R with current I, the field at the center is B = μ₀I/(4R), exactly half that of a complete circle due to the missing half. In this scenario, the arc has radius R = 0.20 m, carries I = 10 A, with μ₀ = 4π × 10⁻⁷ T·m/A. Choice A is correct because it properly calculates: B = (4π × 10⁻⁷ × 10)/(4 × 0.20) = (40π × 10⁻⁷)/0.80 = 50π × 10⁻⁷ = 1.57 × 10⁻⁵ T ≈ 1.6 × 10⁻⁵ T. Choice C is incorrect as it represents half the correct value, suggesting confusion about the geometric factor for semicircles. To help students: derive the semicircle result by integrating the Biot-Savart Law over half a circle, emphasize that the factor of 4 (not 2) in the denominator accounts for the semicircle geometry, and practice comparing full circle and semicircle configurations. Visual aids showing current elements and their field contributions help build intuition.

7

A long, straight wire in vacuum carries $I=12\ \text{A}$ upward. Point $P$ is $d=0.040\ \text{m}$ from the wire. Use Biot-Savart result $B=\dfrac{\mu_0 I}{2\pi d}$ and $\mu_0=4\pi\times10^{-7}\ \text{T·m/A}$. What is the magnitude of the magnetic field at point $P$ due to the wire?

$1.2\times10^{-4}\ \text{T}$

$6.0\times10^{-5}\ \text{T}$

$3.0\times10^{-5}\ \text{T}$

$6.0\times10^{-6}\ \text{T}$

Explanation

This question tests AP Physics C skills in applying the Biot-Savart Law result for the magnetic field around a long, straight current-carrying wire. The magnetic field at distance d from an infinite straight wire is given by B = (μ₀I)/(2πd), where μ₀ is the permeability of free space. In this scenario, a wire carries I = 12 A upward, and we need to find the field at point P located d = 0.040 m from the wire, with μ₀ = 4π × 10⁻⁷ T·m/A. Choice A is correct because substituting the values gives B = (4π × 10⁻⁷ × 12)/(2π × 0.040) = (48π × 10⁻⁷)/(0.080π) = 48 × 10⁻⁷/0.080 = 600 × 10⁻⁷ = 6.0 × 10⁻⁵ T. Choice B is incorrect because it appears to have an extra factor of 10 error, possibly from miscalculating the decimal placement. To help students: Emphasize canceling π terms systematically, practice powers of 10 arithmetic, and encourage checking units throughout calculations. Drawing the wire configuration with field lines circling the wire helps visualize the problem geometry.

8

A long, straight wire in vacuum carries $I=12\ \text{A}$ upward. Point $P$ is $d=4.0\ \text{mm}$ from the wire. Use $B=\dfrac{\mu_0 I}{2\pi d}$ and $\mu_0=4\pi\times10^{-7}\ \text{T·m/A}$. What is the magnitude of the magnetic field at point $P$ due to the wire?

$6.0\times10^{-5}\ \text{T}$

$6.0\times10^{-6}\ \text{T}$

$6.0\times10^{-3}\ \text{T}$

$6.0\times10^{-4}\ \text{T}$

Explanation

This question tests AP Physics C skills in applying Ampère's Law to calculate magnetic fields from infinite straight current-carrying wires. The magnetic field around a long straight wire is given by B = μ₀I/(2πd), where μ₀ is the permeability of free space, I is the current, and d is the perpendicular distance from the wire. In this scenario, the current I = 12 A flows upward through the wire, and the field is calculated at point P located d = 4.0 mm = 0.004 m from the wire. Choice A is correct because it accurately applies the formula: B = (4π×10⁻⁷)(12)/(2π×0.004) = 48π×10⁻⁷/(0.008π) = 48×10⁻⁷/0.008 = 6.0×10⁻⁴ T. Choice B is incorrect because it appears to have an extra factor of 10⁻¹ error, possibly from mishandling the millimeter to meter conversion. To help students: Always convert units before substituting (mm to m), use the convenient form μ₀/(2π) = 2×10⁻⁷ T·m/A for faster calculations, and check that the field strength increases as you get closer to the wire.