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Flashcards · 9630 · A Level Topic 8

Electric fields and capacitance (A Level) flashcards

21 cards on A Level Topic 8, subtopics 3.8.1 to 3.8.4. Pick a subtopic or study them all.

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3.8.1 Coulomb's law

Coulomb's law
The force between two point charges is proportional to the product of the charges and inversely proportional to the square of their separation: F = Q₁Q₂/(4πε₀r²). Like charges repel; unlike attract.
Value of ε₀ and of 1/(4πε₀)
ε₀ = 8.85 × 10⁻¹² F m⁻¹, so 1/(4πε₀) ≈ 8.99 × 10⁹ N m² C⁻². Air can be treated as a vacuum.
Where is the charge on a charged sphere taken to act?
At its centre, so r is measured from the centre of the sphere.
Electrostatic vs gravitational force between a proton and an electron
The electrostatic force is about 2.3 × 10³⁹ times larger. Both are inverse-square, so the ratio does not depend on r; gravity is negligible between subatomic particles.
Charges +1.5 μC and +2.5 μC are 0.20 m apart in air. Force?
F = (1.5 × 10⁻⁶ × 2.5 × 10⁻⁶) ÷ (4π × 8.85 × 10⁻¹² × 0.20²) = 0.84 N, repulsive.

3.8.2 Electric field strength

Electric field strength E
The force per unit positive charge at a point: E = F/Q. A vector, in N C⁻¹ (equivalent to V m⁻¹).
Field strength in a uniform field and in a radial field
Uniform (parallel plates): E = V/d. Radial (point charge Q): E = Q/(4πε₀r²).
Derive E = V/d for parallel plates
Work done moving charge Q across the gap: W = Fd = QEd. Also W = QV. So QEd = QV and E = V/d.
Path of a charged particle entering a uniform field at right angles
Constant velocity along the plates (no force that way) and constant acceleration a = QE/m across them, so the path is a parabola.
Field lines between charged parallel plates
Parallel, equally spaced straight lines at right angles to the plates, from positive to negative, bending slightly outwards only at the edges.

3.8.3 Electric potential

Absolute electric potential at a point
The energy transferred per coulomb of positive test charge when a small test charge is moved from infinity to that point. Zero at infinity. Unit V (J C⁻¹).
Potential in a radial field, and work done moving a charge
V = Q/(4πε₀r), keeping the sign of Q. ΔW = QΔV.
Equipotential surface (electric)
A surface on which every point has the same potential. No work is done moving a charge along it.
How are E and V related on graphs against r?
E = −ΔV/Δr: E is the gradient of the V–r graph. The area under the E–r graph between two radii gives the potential difference.
Potential vs field strength
Potential is a scalar varying as 1/r; field strength is a vector varying as 1/r². A point of zero potential need not have zero field.

3.8.4 Capacitors

Capacitance
The charge stored per unit potential difference: C = Q/V. Unit farad, F (C V⁻¹).
Capacitance of a parallel-plate capacitor
C = Aε₀ε_r/d, where A is the overlap area, d the plate separation and ε_r the relative permittivity of the dielectric.
Energy stored by a capacitor
E = ½QV = ½CV² = Q²/(2C): the area under a graph of Q against V.
How does a dielectric of polar molecules increase capacitance?
In the field each molecule feels a couple and rotates to align. The aligned molecules produce a field opposing the applied field, so the net field falls. For the same Q the p.d. falls, so C = Q/V rises.
A dielectric is inserted into a capacitor. Isolated vs still connected to the battery
Isolated: Q stays fixed and V falls. Connected: V stays fixed and Q rises.
Energy stored by 100 μF charged to 10 V
½CV² = ½ × 100 × 10⁻⁶ × 10² = 5.0 × 10⁻³ J.