Electric Fields of Charge Distributions
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AP Physics C: Electricity and Magnetism › Electric Fields of Charge Distributions
A precision ion trap uses a uniformly charged thin ring (insulating) of radius $R=0.12\ \text{m}$ carrying total charge $Q=+3.0\ \text{nC}$. A test point $P$ lies on the ring’s axis a distance $z=0.09\ \text{m}$ from the center. Consider the setup described above. The field is needed to estimate the axial restoring force on ions near the center. Use the standard on-axis ring result and give direction along $\pm\hat{z}$ in N/C.
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qz}{(z^2+R^2)^{3/2}},(-\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{(z^2+R^2)},(+\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qz}{(z^2+R^2)^{3/2}},(+\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{z^2},(+\hat{z})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically the standard result for a uniformly charged ring on its axis (AP Physics C: Electricity and Magnetism). Electric fields from ring distributions exhibit axial symmetry, where radial components cancel and only the axial component remains. In this scenario, the setup involves a charged ring with a test point on its axis, requiring the well-known on-axis formula. Choice B is correct because it applies the standard ring formula E = (1/4πε₀)(Qz/(z² + R²)^(3/2)), which accounts for the z/r factor from the axial component of each charge element's contribution. Choice A is incorrect because it treats the ring as a point charge at distance z, missing the geometric factor from the ring's finite size. To help students: Derive the ring formula from first principles to understand the (z² + R²)^(3/2) term, emphasize how symmetry eliminates radial components, and practice recognizing when to use memorized results. Watch for: confusing the ring formula with disk or sphere formulas, forgetting the z factor in the numerator.
A charged-particle detector is shielded using a uniformly charged insulating disk of radius $R=0.20\ \text{m}$ with surface charge density $\sigma=+4.0\ \mu\text{C/m}^2$. The disk lies in the $xy$-plane centered at the origin, and point $P$ is on the axis at $z=0.10\ \text{m}$. Consider the setup described above. The field at $P$ is needed to estimate deflection of slow electrons. Use the finite-disk axial field expression and state direction along $\pm\hat{z}$ in N/C.
$E=\dfrac{\sigma}{\epsilon_0}\left(1-\dfrac{z}{\sqrt{z^2+R^2}}\right)(+\hat{z})$
$E=\dfrac{\sigma}{2\epsilon_0}\left(1-\dfrac{z}{\sqrt{z^2+R^2}}\right)(+\hat{z})$
$E=\dfrac{\sigma}{2\epsilon_0}\left(1-\dfrac{R}{\sqrt{z^2+R^2}}\right)(+\hat{z})$
$E=\dfrac{\sigma}{2\epsilon_0}\left(1-\dfrac{z}{\sqrt{z^2+R^2}}\right)(-\hat{z})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically the finite disk formula derived by integrating ring contributions (AP Physics C: Electricity and Magnetism). Electric fields from uniformly charged disks require integrating concentric ring contributions, yielding a result that approaches σ/2ε₀ for infinite planes. In this scenario, the setup involves a charged disk with surface charge density σ and a point on its axis. Choice A is correct because it uses the standard disk formula E = (σ/2ε₀)[1 - z/√(z² + R²)], which results from integrating ring contributions from radius 0 to R. Choice B is incorrect because it has an extra factor of 2, suggesting confusion with the infinite plane result σ/ε₀. To help students: Show how the disk formula emerges from integrating rings, demonstrate the limiting cases (z→0 gives σ/2ε₀, z→∞ gives point charge behavior), and practice recognizing charge distribution geometries. Watch for: using the wrong formula for the geometry, confusion about when to use σ/2ε₀ versus σ/ε₀.
A charged ring electrode for a mass spectrometer is modeled as a thin ring of radius $R=0.050\ \text{m}$ with total charge $Q=-8.0\ \text{nC}$. The measurement point $P$ lies on the axis at $z=0.10\ \text{m}$ from the center. Consider the setup described above. The field direction determines whether ions are pushed toward or away from the ring. Use the on-axis ring field formula and report direction along $\pm\hat{z}$ in N/C.
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{z^2},(+\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qz}{(z^2+R^2)^{3/2}},(-\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{(z^2+R^2)},(-\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qz}{(z^2+R^2)^{3/2}},(+\hat{z})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically the ring formula with negative charge (AP Physics C: Electricity and Magnetism). Electric fields from negatively charged rings point toward the ring, requiring careful application of the standard formula with proper sign. In this scenario, the setup involves a negatively charged ring with a test point on its positive z-axis. Choice C is correct because the negative charge creates a field pointing toward the ring (negative z-direction for positive z), using E = |Q|z/(4πε₀(z² + R²)^(3/2)) with -ẑ direction. Choice A is incorrect because it gives +ẑ direction, which would apply to positive charge but not negative charge. To help students: Reinforce that the ring formula's direction depends on charge sign and position relative to the ring, practice visualizing field directions before calculating, and check that results match physical intuition. Watch for: automatically using +ẑ without considering charge sign, confusion about field direction on different sides of the ring.
A solid insulating sphere of radius $R=0.10\ \text{m}$ is uniformly charged with total charge $Q=-5.0\ \text{nC}$ for an electrostatics lab. A sensor is placed at $r=0.050\ \text{m}$ from the center (inside). Consider the setup described above. The goal is to compare measured field to the Gauss’s law prediction. Use the inside-sphere result and give direction $\pm\hat{r}$ in N/C.
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qr}{R^3}(-\hat{r})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{R^2}(-\hat{r})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{r^2}(-\hat{r})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qr}{R^3}(+\hat{r})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically Gauss's Law inside a uniformly charged sphere with negative charge (AP Physics C: Electricity and Magnetism). Electric fields inside uniformly charged spheres point radially inward for negative charge, with magnitude increasing linearly with radius. In this scenario, the setup involves a point inside a negatively charged sphere where Gauss's Law determines both magnitude and direction. Choice B is correct because for negative total charge Q, the field inside is E = |Q|r/(4πε₀R³) pointing radially inward (-r̂ direction), combining the r/R³ dependence with the proper direction for negative charge. Choice C is incorrect because it gives radially outward direction (+r̂), which would apply to positive charge but contradicts the negative charge given. To help students: Emphasize that Gauss's Law gives field magnitude while charge sign determines direction, practice with both positive and negative charges, and verify directions match the expected behavior of test charges. Watch for: forgetting to account for charge sign in determining direction, confusion between magnitude formulas and directional considerations.
A polymer sphere of radius $R=0.050\ \text{m}$ is manufactured with uniform volume charge density $\rho=+2.0\ \mu\text{C/m}^3$ to create a known calibration field. A probe is placed at $r=0.030\ \text{m}$ from the center (inside the sphere). Consider the setup described above. The field is needed to verify Gauss’s law behavior in the bulk material. Assume spherical symmetry and express the field in N/C with direction $\pm\hat{r}$.
$E=\dfrac{\rho R^3}{3\epsilon_0 r^2}(+\hat{r})$
$E=\dfrac{\rho r}{3\epsilon_0}(-\hat{r})$
$E=\dfrac{\rho r}{3\epsilon_0}(+\hat{r})$
$E=\dfrac{\rho r}{\epsilon_0}(+\hat{r})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically using Gauss's Law for a uniformly charged sphere (AP Physics C: Electricity and Magnetism). Electric fields inside uniformly charged spheres vary linearly with radius due to the enclosed charge increasing as r³ while the Gaussian surface area increases as r². In this scenario, the setup involves a point inside a uniformly charged sphere with volume charge density ρ. Choice A is correct because Gauss's Law with a spherical Gaussian surface of radius r gives E(4πr²) = ρ(4πr³/3)/ε₀, yielding E = ρr/3ε₀ radially outward. Choice C is incorrect because it's missing the factor of 1/3 that comes from the volume integral of the enclosed charge. To help students: Emphasize the importance of correctly calculating enclosed charge for Gaussian surfaces, practice applying Gauss's Law to spherical symmetry, and understand why the field increases linearly inside. Watch for: forgetting the 1/3 factor from sphere volume, confusion between inside and outside formulas.
A microfluidics experiment uses a thin insulating rod of length $L=0.60\ \text{m}$ with uniform charge density $\lambda=-2.5\ \mu\text{C/m}$ centered on the origin along the $x$-axis. A droplet is located at point $P$ on the perpendicular bisector at $y=0.40\ \text{m}$. Consider the setup described above. The field is needed to predict droplet acceleration near the rod. Use symmetry to determine the direction and give $E$ in N/C.
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{\lambda L}{y\sqrt{y^2+(L/2)^2}},(+\hat{y})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{\lambda L}{y^2},(-\hat{y})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{\lambda L}{y\sqrt{y^2+(L/2)^2}},(-\hat{y})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{2\lambda}{y},(-\hat{y})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically integrating for a finite line charge with attention to sign (AP Physics C: Electricity and Magnetism). Electric fields from negative charge distributions point toward the charges, requiring careful attention to both magnitude and direction. In this scenario, the setup involves a negatively charged rod with a test point on the perpendicular bisector. Choice B is correct because the negative charge (λ < 0) creates a field pointing toward the rod (negative y-direction), and the magnitude formula E = |λ|L/(4πε₀y√(y² + (L/2)²)) gives the correct result with -ŷ direction. Choice A is incorrect because it gives +ŷ direction, which would be correct for positive charge but wrong for negative charge. To help students: Emphasize that field direction depends on charge sign (away from positive, toward negative), practice keeping track of signs throughout calculations, and verify directions make physical sense. Watch for: forgetting that negative charges reverse field direction, sign errors in setting up integrals.
A uniformly charged insulating sphere of radius $R=0.080\ \text{m}$ carries total charge $Q=+6.0\ \text{nC}$ for a high-voltage safety test. A field meter is located at $r=0.20\ \text{m}$ from the center (outside the sphere). Consider the setup described above. The field magnitude is required to set safe separation distances. Treat the external field as that of a point charge at the center and give direction $\pm\hat{r}$ in N/C.
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{r^2}(-\hat{r})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{r^2}(+\hat{r})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{R^2}(+\hat{r})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qr}{R^3}(+\hat{r})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically applying Gauss's Law outside a uniformly charged sphere (AP Physics C: Electricity and Magnetism). Electric fields outside any spherically symmetric charge distribution behave as if all charge were concentrated at the center, regardless of the internal distribution. In this scenario, the setup involves a point outside a uniformly charged sphere, where the total charge Q matters but not the detailed distribution. Choice A is correct because outside the sphere (r > R), Gauss's Law gives the same result as a point charge: E = Q/(4πε₀r²) radially outward. Choice C is incorrect because it uses the inside-sphere formula E ∝ r, which only applies for r < R. To help students: Stress that Gauss's Law shows all spherically symmetric distributions look like point charges from outside, practice identifying when to use inside versus outside formulas, and reinforce the r < R and r > R conditions. Watch for: using the wrong formula for the region, confusion about field continuity at r = R.
In a particle-beam alignment rig, a thin insulating rod of length $L=0.40\ \text{m}$ lies along the $x$-axis from $x=-0.20$ m to $x=+0.20$ m with uniform linear charge density $\lambda=+6.0\ \mu\text{C/m}$. A sensor at point $P$ is on the perpendicular bisector at $y=0.30$ m. Consider the setup described above. Neglect end effects beyond the finite rod and use superposition to find the field at $P$ in N/C. Symmetry implies horizontal components cancel, leaving only a $+\hat{y}$ or $-\hat{y}$ direction depending on sign. The engineering goal is to predict sensor saturation during calibration.
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{2\lambda}{y},(+\hat{y})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{\lambda L}{y^2},(+\hat{y})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{\lambda L}{y\sqrt{y^2+(L/2)^2}},(-\hat{y})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{\lambda L}{y\sqrt{y^2+(L/2)^2}},(+\hat{y})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically using integration for a finite line charge (AP Physics C: Electricity and Magnetism). Electric fields from continuous charge distributions require integrating contributions from infinitesimal charge elements, with the field direction determined by symmetry. In this scenario, the setup involves a uniformly charged rod along the x-axis with a test point on the perpendicular bisector, where horizontal components cancel by symmetry. Choice C is correct because it properly integrates dE = (λdx)/(4πε₀r²) with r = √(y² + x²) and includes the vertical component factor y/r, yielding the expression with √(y² + (L/2)²) in the denominator. Choice A is incorrect because it treats the rod as a point charge at distance y, ignoring the extended nature of the distribution. To help students: Emphasize identifying symmetry to simplify vector addition, practice setting up integrals with proper distance expressions, and ensure understanding of when components cancel. Watch for: forgetting to include directional components in the integral, treating extended objects as point charges.
An electrostatic sensor is tested near a uniformly charged thin ring of radius $R=0.30\ \text{m}$ carrying total charge $Q=+2.0\ \text{nC}$. The sensor is placed far on the axis at $z=3.0\ \text{m}$ to check the far-field approximation. Consider the setup described above. The field is needed to confirm the ring behaves like a point charge at large distances. Use the ring’s on-axis expression and indicate direction along $\pm\hat{z}$ in N/C.
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qz}{(z^2+R^2)^{3/2}},(+\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Qz}{(z^2+R^2)^{3/2}},(-\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{z^2},(+\hat{z})$
$E=\dfrac{1}{4\pi\epsilon_0}\dfrac{Q}{(z^2+R^2)},(+\hat{z})$
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically verifying the far-field limit of a charged ring (AP Physics C: Electricity and Magnetism). Electric fields from any finite charge distribution approach point-charge behavior at large distances, providing a useful approximation and consistency check. In this scenario, the setup involves a charged ring with observation point at z >> R, where the ring should behave like a point charge. Choice A is correct because the exact ring formula E = Qz/(4πε₀(z² + R²)^(3/2)) remains valid at all distances and naturally reduces to Q/(4πε₀z²) when z >> R, maintaining the +ẑ direction for positive charge. Choice C is incorrect because it jumps directly to the point-charge approximation Q/(4πε₀z²), which while approximately correct, isn't the exact expression requested. To help students: Show how complex formulas reduce to simple limits, practice Taylor expansions for far-field approximations, and emphasize when exact versus approximate formulas are appropriate. Watch for: prematurely using approximations when exact results are needed, confusion about when limiting cases apply.
A calibration source is a uniformly charged solid sphere of radius $R=0.050,\text{m}$ with volume charge density $\rho=+2.0,\mu\text{C/m}^3$; the electric field at a point $r=0.020,\text{m}$ from the center is needed to set detector gain in $\text{N/C}$. The sphere is isolated in vacuum and centered at the origin. Assume the charge remains uniformly distributed throughout the volume. Consider the setup described above. Using Gauss's Law, determine the electric field inside the charged sphere.
$E=\dfrac{\rho R^3}{3\varepsilon_0 r^2}$, radially outward
$E=\dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{r^2}$, radially outward
$E=\dfrac{\rho r}{3\varepsilon_0}$, radially outward
$E=\dfrac{\rho r}{3\varepsilon_0}$, radially inward
Explanation
This question tests AP Physics C skills on electric fields from charge distributions, specifically using Gauss's Law for a uniformly charged sphere (AP Physics C: Electricity and Magnetism). Gauss's Law relates electric flux through a closed surface to enclosed charge, making it ideal for problems with high symmetry. In this scenario, we have a uniformly charged solid sphere with volume charge density ρ, and we need the field at r < R inside the sphere. Choice C is correct because applying Gauss's Law with a spherical Gaussian surface of radius r < R gives E·4πr² = Q_enclosed/ε₀ = ρ(4πr³/3)/ε₀, yielding E = ρr/3ε₀ radially outward. Choice B incorrectly uses the total charge Q = ρ(4πR³/3) instead of just the enclosed charge. To help students: Emphasize that only charge within the Gaussian surface contributes to the field, practice identifying Q_enclosed for different charge distributions. Watch for: using total charge instead of enclosed charge, forgetting the r³ dependence of enclosed volume.