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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.
Revise Electric fields and capacitance further
- Study guideOxfordAQA International AS and A-level Physics: Coulomb's law and electric field strength (9630)
- Revision notesOxfordAQA International AS and A-level Physics: Coulomb's law and electric field strength (9630) – Revision Notes
- Practice questionsOxfordAQA International AS and A-level Physics: Coulomb's law and electric field strength (9630) – Practice Questions