AP Unit 10 Problems
17 learning problems for Unit 10. Draw the situation, name the model and explain why each step follows. These are authored practice, with worked solutions on a separate page.
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Problem 1
Two small beads A and B are 0.20 m apart. A has lost 2.0 × 10¹² electrons and B has gained 1.0 × 10¹² electrons. Each bead’s diameter is 1 mm. Treat them in air as point charges.
Part a
Find the charges on A and B, explain the sign of each, and justify the point-charge approximation. Include the charge of a neutron and why the charges are quantized.
Part b
Find the magnitude and direction of each mutual force. Then predict the force factor if both charge magnitudes double and the separation triples. Also explain what changes if only B’s charge sign reverses.
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Problem 2
A student claims that electricity must control planetary orbits because it is much stronger than gravity between two protons. Use mp = 1.67 × 10⁻²⁷ kg and the constants in the teacher guide.
Part a
Derive FE/Fg for a proton pair, calculate it, and explain why the planetary claim does not follow. Explain how electric interactions also relate to the normal force of a table.
Part b
For fixed free charges in an ideal uniform linear dielectric with κ = 5, predict the electric-force factor relative to vacuum. Explain what permittivity measures, polarization, the role of composition, and why an insulator can respond without conducting across the sample.
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Problem 3
In an isolated apparatus, an initially neutral plastic rod is rubbed with an initially neutral cloth. The rod then has −12 nC. It is brought near an initially neutral insulated metal can without touching.
Part a
Find the cloth charge and the number of electrons transferred during rubbing. Explain why rubbing changes net charge but bringing the rod nearby alone does not change the can’s net charge.
Part b
Draw and describe the signs on the can’s near and far regions, then predict how a neutral insulating strip could also be attracted.
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Problem 4
A neutral conducting sphere is insulated from Earth. A positive rod is held near it. A switch can briefly connect the sphere to Earth.
Part a
Design a sequence that leaves the sphere with negative net charge without touching the rod to it. Illustrate the charge distributions and identify electron-transfer direction and the step at which net charge changes.
Part b
In a separate contact experiment, remove the rod and all other asymmetric external fields. Two identical metal spheres, initially −4 nC and +10 nC, touch in a symmetric environment while isolated from Earth, then separate. Find their final charges and each signed charge change.
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Problem 5
Sources +2.0 nC at (−0.10 m, 0) and +2.0 nC at (+0.10 m, 0) surround point P = (0, 0.10 m).
Part a
Draw the separate source-field arrows at P and calculate the net field. Explain what arrow length represents in a vector map and what field-line density would imply. Then reverse only the right-hand source to −2.0 nC: draw its new source-field arrow and calculate the new net field at P.
Part b
Find the force on a small −3.0 nC test charge at P and compare it with the force on +3.0 nC at the same point in the original two-positive-source configuration. Explain why making either test charge nonperturbing matters.
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Problem 6
An isolated solid conducting sphere has radius R = 0.050 m and net charge +5.0 nC. It is in electrostatic equilibrium.
Part a
Calculate the field at r = 0.030 m and r = 0.10 m from its center. Sketch E magnitude against r and state the direction at its surface. State where the sphere’s excess charge resides at equilibrium.
Part b
Explain why an internal field would contradict equilibrium in the metal. Replace the sphere with an insulating sphere carrying excess charge through its volume: can you conclude its internal field is zero?
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Problem 7
A +3.0 nC charge and a −2.0 nC charge are slowly separated from 0.10 m to 0.25 m. Choose U = 0 at infinite separation.
Part a
Find Ui, Uf, and ΔU. State the external work and electric-force work if the speeds stay negligibly small.
Part b
Sketch the U versus r curve for this pair, label zero at infinity, and compare the energy change if both separations were doubled.
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Problem 8
Three point charges +q, +q, and −q occupy an equilateral triangle of side a.
Part a
Derive the total assembly energy by listing the pairs. For q = 4.0 nC and a = 0.20 m, calculate it.
Part b
The negative charge is moved infinitely far away while the two positive charges stay fixed. Find ΔU and the slow external work symbolically and numerically.
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Problem 9
Two fixed sources +6.0 nC and −2.0 nC are each 0.20 m from an observation point P. Use zero potential at infinity.
Part a
Find V(P), then the interaction energy of a +3.0 nC test charge at P. Explain why source-field arrows alone cannot be added as potential arrows.
Part b
A 9 V battery moves 2.0 mC of positive charge internally from its low-potential terminal to its high-potential terminal. Find the energy increase and name its source. Separately, two unequal isolated metal spheres touch: what equality must hold after redistribution?
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Problem 10
A map shows vertical equipotentials 24 V at x = 0 cm, 18 V at x = 1 cm, and 12 V at x = 2 cm. Farther right, 6 V and 0 V contours are 2 cm apart. The lines are smooth and locally parallel.
Part a
Draw local field arrows in both regions with relative magnitudes. Explain their orientation, direction, and whether a field component lies along a contour.
Part b
A −2.0 μC charge moves from the 24 V line to the 12 V line. Find ΔU and describe its initial electric-force direction. What is the work if it instead moves between two points on the 18 V line?
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Problem 11
A parallel-plate capacitor has plate overlap area 0.030 m², a uniform dielectric κ = 2.0, and plate separation 1.5 mm. It is connected to an ideal 10 V battery. Neglect edges.
Part a
Find C, each plate’s charge, central field magnitude and direction, and stored energy. Explain why Q is not the capacitor’s net charge.
Part b
Construct a quantitative graph of capacitor ΔV (V) against Q (nC), using numerical scales and plotting (0, 0), (1.77 nC, 5 V), and (3.54 nC, 10 V) as it charges from zero. Explain why its area is the stored energy ½QΔV and distinguish that from the work supplied by the constant 10 V battery. Then predict C and U if overlap area doubles with the battery still connected.
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Problem 12
An initially air-gap capacitor has C₀ = 200 pF and is charged to 20 V. A κ = 4 dielectric can fully fill the gap without changing geometry. A separate particle experiment uses a uniform 500 N/C vertical field.
Part a
Compare final charge, voltage, field factor, and stored energy for dielectric insertion with the battery disconnected and with it connected. Explain the induced field direction.
Part b
A particle with q = −1.0 μC and m = 2.0 × 10⁻⁴ kg enters horizontally at 4.0 m/s into the downward 500 N/C field over horizontal length 0.20 m. Create a qualitative y-versus-x graph of the path with labeled axes (x rightward, y upward) and indicate its horizontal initial tangent. Then find the electric acceleration, transit time, and deflection. Neglect gravity and edge fields, and assume no plate collision.
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Problem 13
A proton starts from rest at a 300 V equipotential and reaches a 100 V equipotential under only electric forces. Use mp = 1.67 × 10⁻²⁷ kg.
Part a
Find ΔU, final kinetic energy in joules and electron-volts, and final speed. Draw energy bars that represent the change.
Part b
A slow external agent instead transports the same proton from 100 V to 300 V at unchanged speed. Find Wext and explain why final kinetic energy no longer follows −qΔV alone.
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Problem 14
A positively charged particle has charge +q, mass m, initial speed v₀, and initial potential V₀. It moves in one dimension along x into monotonically increasing electric potential, with no transverse velocity and only electric forces acting. The uphill region extends far enough that the particle eventually turns.
Part a
Derive the potential at the one-dimensional turning point and explain the meaning of a calculated negative final kinetic energy at a proposed higher potential.
Part b
Two particles have equal mass and equal initial speed, but charges +q and +2q. Compare their maximum potential increases. Then describe a negative particle’s energy change moving to higher potential.
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Problem 15
Students use a voltmeter to map a conductive-paper analogue. Along a horizontal line, measured values are V(0.00 m) = 8.0 V, V(0.02 m) = 6.0 V, V(0.04 m) = 4.0 V, and V(0.06 m) = 2.0 V. Each endpoint voltage difference has uncertainty ±0.10 V and each endpoint separation ±0.002 m.
Part a
Construct V versus x, estimate the average field over the whole interval, and give a conservative relative uncertainty using δE/E ≈ δ(ΔV)/|ΔV| + δ(Δx)/Δx. State a control and an assumption of this map.
Part b
Draw equipotentials and field arrows consistent with these data if the region is uniform vertically. Predict force on q = −2.0 μC and ΔU if it moves from x = 0 to x = 0.06 m under a corresponding static source field.
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Problem 16
A student measures a broad-plate capacitor with fixed overlap area A = 0.020 m² and uniform dielectric. Measurements are d = 1.0, 2.0, 4.0 mm and C = 354, 177, 88.5 pF respectively. Lead capacitance is negligible.
Part a
Choose a graph that linearizes the geometry relation, construct it with numerical scales and units, plot the transformed data, fit a line, determine its slope, and infer κ. Outline how to measure C versus d with a capacitance meter, including one control, one repeat strategy, and one likely systematic error.
Part b
At d = 2.0 mm, charge the capacitor to 10 V, disconnect it, and then double d. Find final Q, V, E, and U. Explain the charge conservation and external energy input in a slow separation.
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Problem 17
Two fixed charges +Q sit at x = −a and x = +a. A small charge +q is placed at the origin. Ignore gravity; the sources stay fixed. Choose potential zero at infinity.
Part a
Find the source field and potential at the origin, and the interaction energy associated with adding q there. Explain why the field and potential results do not conflict.
Part b
Give q a small initial velocity along the perpendicular y axis. If it eventually reaches very far away, derive its final speed in terms of m, vi, Q, q, and a. What can you say about its kinetic-energy change before knowing its travel time?
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More chapter problems
Try these problems before opening the solutions. Show the physical model, your calculation or sketch, and the reason your conclusion follows.
Does zero net charge remove the charge property?
A sample contains N initially neutral atoms, each with 6 protons, 6 electrons and 6 neutrons. It later loses exactly 3.0 × 10⁹ electrons, with no nuclear change. N is large enough to supply that count. Use e = 1.60 × 10⁻¹⁹ C.
(a) Evaluate the claim “charge is a fundamental property only of matter with nonzero net charge.” Explain the role of zero net charge for this sample and state whether neutral matter and neutrons are excluded from the fundamental charge description.
(b) State the signed charge of one electron, one proton and one neutron. Use all three values to calculate the initial charge of one atom.
(c) Calculate the sample’s final net charge and the signed charge carried away. Explain why the change is quantized and why a claim that one isolated atom loses a charge of +0.4e by losing electrons is inconsistent with this charging model.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
Polarization or conduction?
A neutral insulator has larger permittivity than another in their common linear-response range. Neither conducts net charge freely across its sample.
(a) Which statement best explains the difference?
Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
Build a spatial map from two sources
Two fixed +2.0 nC point charges are at (−0.10 m,0) and (+0.10 m,0). Consider M = (0,0), N = (0,0.10 m), S = (0,−0.10 m), and R = (0.20 m,0). Use k = 8.99 × 10⁹ N·m²/C²; sources remain unchanged by any test charge.
(a) Calculate the net field vector at all four points. Construct a labeled spatial vector map with a common arrow-length scale for magnitude. Show the two source contributions at N, explain the cancellations or additions at every point, and mark a zero at M rather than assigning it a direction.
(b) Find the initial electric forces on +1.0 nC and −1.0 nC test charges separately placed at N. Explain why the map is unchanged and whether those forces alone specify each complete future trajectory.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
Bring a pair together from infinity
A +3.0 nC point charge is held fixed. A second point charge initially infinitely far away is brought to r = 0.20 m in vacuum. Compare second charges +2.0 nC and −2.0 nC in separate trials. Choose pair U = 0 at infinity and use k = 8.99 × 10⁹ N·m²/C².
(a) For an external quasistatic assembly with negligible kinetic-energy change, determine the final U, the work done by the external agent from infinity, and the electric-force work in each trial. Explain each external-work sign by relating the agent’s force to the displacement.
(b) Construct U-versus-r graphs for the two pairs on common quantitative axes. Plot at least r = 0.20, 0.40 and 0.80 m, label values and units, and describe the r → ∞ limit. Distinguish this scaling from the force magnitude.
(c) In a different opposite-sign trial, remove the agent and release the second charge from rest at infinity in the idealized limit. At r = 0.20 m, calculate ΔK and W_ext. Explain why the negative final U is not the external work for this free motion.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
Read a field and predict actual motion
In a uniform static region, vertical equipotentials are 30 V at x = 0, 20 V at x = 0.020 m, and 10 V at x = 0.040 m. A nonperturbing particle has q = −1.0 nC, m = 2.0 × 10⁻⁶ kg and starts at (x,y) = (0.030 m,0) with velocity (0,+0.10 m/s). Ignore gravity and all other forces. The uniform region includes its motion for 0.20 s.
(a) Construct the labeled contour map and a matching field-vector map at several points. Calculate E and state its direction, magnitude uniformity, perpendicularity to contours, and component along a contour.
10.5.B.110.5.B.2.i10.5.B.2.ii10.5.B.2.iii10.5.B.2.iv10.3.A.3.ii
(b) Predict the initial force and acceleration. Calculate the particle’s x and y coordinates at 0.20 s. Add its initial tangent and qualitative curved trajectory to your map, and explain why it does not follow a rightward field arrow.
(c) Use the potential map to calculate ΔU and ΔK for that interval. Check ΔK from the velocity change and explain why moving between any two points on the same contour gives zero net electric work.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →
Is the plate field uniform everywhere?
Two broad horizontal conducting plates have uniform equal-and-opposite charge in the idealized model. The upper plate is at 12 V and the lower at 0 V. Separation d = 0.020 m and lateral size is 1.0 m. Points A, B and C lie far from all edges: A is near the upper plate, B is midway, and C near the lower plate. Point D is beside a finite plate end. Use the central approximation, air κ ≈ 1, and no other forces.
(a) Calculate the central field. Draw arrows at A, B and C on one magnitude scale and state whether both magnitude and direction are constant. Explain the plate-sign direction and why A is not assigned a larger field just because it is nearer the upper plate.
(b) Sketch the qualitative field near an end of the plates and explain why the constant central field cannot be assigned automatically at D. State the geometric and location conditions needed for your central approximation, and label any edge sketch direction-only if its arrow lengths have no common magnitude scale.
(c) A particle with q = −2.0 nC and m = 4.0 × 10⁻⁶ kg enters the central gap at the midpoint with horizontal speed 0.50 m/s and zero vertical speed. Use x right and y upward. Find acceleration and its deflection over 0.080 m of central travel. Check for plate collision, and state why this calculation does not determine its path through an entry or exit fringe.
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Worked solution and rubric →Revisit the explanation →Revisit the explanation →Read the relevant lesson →