Chapter revision
Revision summary
Key ideas, equations and common mistakes. Open any topic below for the full explanation.
State the source, test charge, direction and reference. Then select a force, field, potential or energy equation appropriate to that quantity.
Point charges: signs and inverse powers
Force magnitude: F = K|Qq|/r2
Outward-positive field: Er = KQ/r2
Test-charge force: Fr = qEr
V = KQ/r; UE = KQq/r = qV
These point-charge equations use free space or air and centre separation r. Like signs repel and unlike signs attract. The source determines E and V; test-charge sign then determines its force and pair energy. Potential is scalar, while fields and forces add as vectors.
Potential is external work per unit small positive test charge brought from infinity without a kinetic-energy change. With the isolated-source zero at infinity, V follows source sign and UE follows the product of the two signs.
Slow prescribed motion: Wexternal = ΔUE
Field work = -ΔUE
Field-only motion: ΔEk = -qΔV
The work and motion statements require the stated fixed-source, negligible-other-transfer conditions. Moving -2.00 nC from +120 to +60.0 V raises its pair energy by +1.20 × 10-7 J.
Use a local gradient and a perpendicular gap
Uniform plates: E = |ΔV|/d
1 V/m = 1 N/C
A tangent slope of -400 V/m gives a +400 N/C component. A chord across a finite interval need not give that local value. Field is perpendicular to equipotentials and points towards decreasing V; a negative charge's force is opposite E.
At the midpoint between two equal positive sources, fields can cancel while potentials add. With equal opposite sources, potentials can cancel while fields reinforce. Zero E and zero V are different conditions.
For plates at +120 and 0 V separated by 0.0300 m, the field is 4000 V/m from the higher to lower potential. Use the perpendicular gap, not plate length. A chosen 0 V label does not imply an Earth connection.
Calculate motion in components
With electric force alone, a = qE/m. An electron is accelerated opposite E. In the supplied transverse-entry model, x = uxt and y = (1/2)ayt2, with vx unchanged. Transit is 3.00 ns, exit deflection is 3.16 mm and exit vy is 2.11 × 106 m/s upward. This is inside the 15.0 mm half-gap.
After the ideal field ends, force-free motion follows the exit tangent. It does not continue curving or reset to horizontal. Revisit the component graphs and energy check to connect the exit state to its assumptions.
Capacitor charge, graph axes and constraints
U = (1/2)QV = Q2/(2C) = (1/2)CV2
Q is the magnitude on either plate. Opposite charges +Q and -Q give zero net pair charge while storing charge separation. Constant C describes a linear capacitor within its operating range.
Q against V has gradient C. V against Q has gradient 1/C, and its area gives stored energy. For the 10.0 microfarad, 12.0 V model, Q = 120 microcoulombs and U = 0.720 mJ.
- Same C, doubled V: Q doubles and U quadruples.
- Same V, doubled C: Q and U double.
- Same Q, doubled C: V and U halve.
State whether a source maintains V or an isolated, non-leaking capacitor retains Q. In the specified initially uncharged, constant-voltage resistive charging model, source transfer VsQ exceeds the final stored energy; account for energy transferred in the resistance.
Quantities and units
| Quantity | Symbol | Unit or meaning |
|---|---|---|
| Source / test charge | Q, q | C; signed charges |
| Elementary-charge magnitude | e | C; electron charge is -e |
| Centre separation | r | m |
| Electric force | F | N; name its recipient |
| Electric field strength | E | N/C = V/m |
| Electric potential | V | V = J/C; stated reference |
| Potential difference | ΔV or V | V; named endpoints |
| Pair potential energy | UE | J; signed with the reference |
| Kinetic energy | Ek | J |
| Permittivity of free space | ε0 | F/m = C2/(N m2) |
| Coulomb factor | K = 1/(4πε0) | N m2/C2 |
| Perpendicular plate gap | d | m |
| Particle mass / velocity | m, v | kg; m/s |
| Capacitance | C | F = C/V |
| Capacitor plate-charge magnitude | Q | C; either plate, not net pair charge |
| Capacitor stored energy | U | J; zero at the uncharged state |
Unit of ε0 = kg-1 m-3 s4 A2
Use 10-9 for nano, 10-6 for micro and 10-3 for milli. Here E means field; energy is U or Ek. The letter C can mean capacitance as a quantity or coulomb as a unit, while F can mean force as a quantity or farad as a unit.
Return to point-charge force and fieldPractise exam questions
Write your answer first, then tick the mark points it makes.
Exam-style question
State how the electric field strength at a point is related to the electric potential there. Two parallel plates 2.0 cm apart have a potential difference of 500 V between them. Calculate the field strength between the plates. [3]
Saved on this browser only. Anyone using this browser can see it.
Exam-style question
Define electric field strength at a point. [2]
Saved on this browser only. Anyone using this browser can see it.
Exam-style question
Calculate the electric field strength 0.10 m from a point charge of +2.0 nC in air. Take 1/(4πε0) = 8.99 x 109 N m2 C-2. [3]
Saved on this browser only. Anyone using this browser can see it.
Exam-style question
An electron enters the uniform electric field between two parallel plates, moving at right angles to the field. Explain why its path between the plates is a parabola. [3]
Saved on this browser only. Anyone using this browser can see it.
Exam-style question
A graph of potential difference V against charge Q for a capacitor is a straight line from the origin to (6.0 mC, 12 V). Use the graph to find the capacitance and the energy stored when the p.d. is 12 V. [3]
Saved on this browser only. Anyone using this browser can see it.
Quick recall
A fixed positive source produces an outward field of 400 N/C at a point. Replace a small -2.00 nC test charge there with +2.00 nC, keeping the source unchanged. What happens?
Review a topic
- Point-charge force and field
- Electric potential and energy
- Field from a potential gradient
- Uniform fields between plates
- Charged-particle motion
- Capacitance and plate charge
- Energy stored in a capacitor