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How do electric fields and potential describe the force on charges?

Electric charge and Coulomb's law, electric field strength, electric potential, and the motion of a charged particle in an electric field.

An SQA Advanced Higher Physics answer on electric fields, covering electric charge and Coulomb's law, electric field strength, electric potential, and the motion of a charged particle accelerated through a potential difference or deflected in a uniform field.

Generated by Claude Opus 4.815 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this key area is asking
  2. Coulomb's law
  3. Electric field strength
  4. Electric potential
  5. Motion of a charged particle
  6. Examples in context
  7. Try this

What this key area is asking

The SQA wants you to use Coulomb's law for the force between point charges, define and use electric field strength, define and use electric potential, and analyse the motion of a charged particle accelerated through a potential difference or deflected in a uniform field.

Coulomb's law

Coulomb's law is the electrostatic analogue of Newton's law of gravitation: both are inverse-square laws, but the electric force can be either attractive or repulsive and is enormously stronger. The constant 14πε0\frac{1}{4\pi\varepsilon_0} replaces GG. Doubling the separation quarters the force, exactly as in gravitation.

Electric field strength

Around a point charge the field strength is E=Q4πε0r2E = \frac{Q}{4\pi\varepsilon_0 r^2}, pointing away from a positive charge. Between two parallel plates the field is uniform and given by E=VdE = \frac{V}{d}, where VV is the potential difference and dd the plate separation. Field lines run from positive to negative, and their spacing shows the field strength. The uniform-field result is the one used for parallel-plate and deflection problems.

Electric potential

Potential describes the energy landscape: a charge qq at potential VV has potential energy qVqV. Unlike gravitational potential, electric potential can be positive (near a positive charge) or negative (near a negative charge). The work done moving a charge between two points is W=qΔVW = q\Delta V, which is the key to accelerating charges.

Motion of a charged particle

Accelerating a charge through a potential difference is how electron guns work, and equating QVQV to 12mv2\tfrac{1}{2}mv^2 gives the final speed. Deflecting a charge in a uniform field is treated exactly like projectile motion: the field provides a constant transverse acceleration a=QEma = \frac{QE}{m}, while the forward velocity is unchanged, so the path is parabolic.

Examples in context

The electron gun in older displays accelerates electrons through a potential difference and deflects them with fields to scan an image, exactly this key area's physics. Inkjet printers charge and deflect droplets in a field to steer them onto the page. Mass spectrometers accelerate ions through a known potential difference to give them a known energy. The van de Graaff generator demonstrates large potentials and the inverse-square field around charged spheres.

Try this

Q1. State the quantity defined as the force per unit positive charge. [1 mark]

  • Cue. The electric field strength, EE.

Q2. Write the relationship for the field strength between two parallel plates a distance dd apart at potential difference VV. [1 mark]

  • Cue. E=VdE = \frac{V}{d}.

Q3. State the kinetic energy gained by a charge QQ accelerated through a potential difference VV. [1 mark]

  • Cue. Ek=QVE_k = QV.

Exam-style practice questions

Practice questions written in the style of SQA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

SQA AH style5 marksTwo point charges of +3.0 μC+3.0\ \mu\text{C} and +5.0 μC+5.0\ \mu\text{C} are 0.20 m0.20\ \text{m} apart in a vacuum. Calculate the electrostatic force between them. Take the permittivity of free space ε0=8.85×1012 F m1\varepsilon_0 = 8.85 \times 10^{-12}\ \text{F m}^{-1}.
Show worked answer →

Use Coulomb's law, F=Q1Q24πε0r2F = \dfrac{Q_1 Q_2}{4\pi\varepsilon_0 r^2}.

Substitute (charges in coulombs): F=3.0×106×5.0×1064π×8.85×1012×0.202F = \dfrac{3.0 \times 10^{-6} \times 5.0 \times 10^{-6}}{4\pi \times 8.85 \times 10^{-12} \times 0.20^2}.

Numerator: 1.5×10111.5 \times 10^{-11}. Denominator: 4π×8.85×1012×0.040=4.45×10124\pi \times 8.85 \times 10^{-12} \times 0.040 = 4.45 \times 10^{-12}.

So F=1.5×10114.45×1012=3.4 NF = \dfrac{1.5 \times 10^{-11}}{4.45 \times 10^{-12}} = 3.4\ \text{N}, repulsive (both charges positive).

Markers reward Coulomb's law, converting microcoulombs to coulombs, squaring the separation, and noting the force is repulsive.

SQA AH style4 marksAn electron is accelerated from rest through a potential difference of 250 V250\ \text{V}. Calculate the kinetic energy and the speed it gains. Take e=1.6×1019 Ce = 1.6 \times 10^{-19}\ \text{C} and me=9.11×1031 kgm_e = 9.11 \times 10^{-31}\ \text{kg}.
Show worked answer →

The work done on the charge equals the energy gained: Ek=QV=eVE_k = QV = eV.

Ek=1.6×1019×250=4.0×1017 JE_k = 1.6 \times 10^{-19} \times 250 = 4.0 \times 10^{-17}\ \text{J}.

Equate to kinetic energy: 12mv2=4.0×1017\tfrac{1}{2}mv^2 = 4.0 \times 10^{-17}, so v=2×4.0×10179.11×1031v = \sqrt{\dfrac{2 \times 4.0 \times 10^{-17}}{9.11 \times 10^{-31}}}.

v=8.8×1013=9.4×106 m s1v = \sqrt{8.8 \times 10^{13}} = 9.4 \times 10^{6}\ \text{m s}^{-1}.

Markers reward using Ek=QVE_k = QV, then equating to 12mv2\tfrac{1}{2}mv^2 to find the speed, both with units.

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