Published by Patrick Mutisya · 14 days ago
In a uniform electric field the electric field vector \$\mathbf{E}\$ has the same magnitude and direction at every point in the region of interest. This idealised situation is useful for understanding the behaviour of charges and for solving many A‑Level problems.
\$\mathbf{E} = \frac{\mathbf{F}}{q}\$
\$\Delta V = -E d\$
\$\mathbf{F}=q\mathbf{E}\$
Coulomb’s law gives the magnitude of the electrostatic force between two point charges \$Q1\$ and \$Q2\$ separated by a distance \$r\$ in free space:
\$F = \frac{Q1 Q2}{4\pi\varepsilon_0 r^{2}}\$
where \$\varepsilon_0 = 8.85\times10^{-12}\,\text{F m}^{-1}\$ is the permittivity of free space.
Consider a large, flat, charged plate of surface charge density \$\sigma\$ (C m⁻²). At a point close to the plate (distance much smaller than the plate dimensions) the field can be approximated as uniform:
\$E = \frac{\sigma}{2\varepsilon_0}\$
Two parallel plates with opposite charge densities produce a uniform field between them:
\$E = \frac{\sigma}{\varepsilon_0} = \frac{V}{d}\$
where \$V\$ is the potential difference between the plates and \$d\$ is the separation.
Problem: Two point charges, \$Q1 = +5.0\,\mu\text{C}\$ and \$Q2 = -3.0\,\mu\text{C}\$, are 0.20 m apart in free space. Calculate the magnitude and direction of the force on each charge.
\$Q1 = 5.0\times10^{-6}\,\text{C},\qquad Q2 = -3.0\times10^{-6}\,\text{C}\$
\$\$F = \frac{|Q1 Q2|}{4\pi\varepsilon_0 r^{2}}
= \frac{(5.0\times10^{-6})(3.0\times10^{-6})}{4\pi(8.85\times10^{-12})(0.20)^{2}}\$\$
\$F \approx 1.35\,\text{N}\$
| Quantity | Formula | Units |
|---|---|---|
| Electric field (uniform) | \$E = \dfrac{V}{d}\$ | V m⁻¹ (N C⁻¹) |
| Coulomb force | \$F = \dfrac{Q1 Q2}{4\pi\varepsilon_0 r^{2}}\$ | N |
| Force on a charge in a field | \$\mathbf{F}=q\mathbf{E}\$ | N |
| Potential difference in uniform field | \$\Delta V = -E d\$ | V |