Published by Patrick Mutisya · 14 days ago
Recall and use the expression
\$E = \frac{Q}{4\pi\varepsilon_0 r^{2}}\$
to calculate the electric field strength due to a point charge in free space.
The expression for the electric field of a point charge follows from Coulomb’s law for the force between two point charges:
\$F = \frac{1}{4\pi\varepsilon_0}\frac{|Qq|}{r^{2}}\$
Dividing the force by a small positive test charge \$q\$ gives the field:
\$E = \frac{F}{q} = \frac{Q}{4\pi\varepsilon_0 r^{2}}\$
Direction is given by the unit vector \$\hat{r}\$ pointing away from a positive \$Q\$ (or toward a negative \$Q\$):
\$\vec{E} = \frac{Q}{4\pi\varepsilon_0 r^{2}}\,\hat{r}\$
Problem: A point charge of \$+5.0\ \mu\text{C}\$ is located at the origin. Find the magnitude of the electric field at a point \$0.20\ \text{m}\$ from the charge.
Solution:
\$E = \frac{5.0\times10^{-6}}{4\pi(8.854\times10^{-12})(0.20)^{2}}\$
\$\$E \approx \frac{5.0\times10^{-6}}{4\pi(8.854\times10^{-12})(0.04)}
\approx 2.24\times10^{5}\ \text{N C}^{-1}\$\$
| Symbol | Quantity | SI Unit | Typical \cdot alue / Note |
|---|---|---|---|
| \$E\$ | Electric field strength | N C⁻¹ (or V m⁻¹) | Calculated from \$Q\$, \$r\$, \$\varepsilon_0\$ |
| \$Q\$ | Point charge | C | Can be positive or negative |
| \$r\$ | Radial distance from charge | m | Must be measured from the exact location of the point charge |
| \$\varepsilon_0\$ | Permittivity of free space | C² N⁻¹ m⁻² | 8.854 × 10⁻¹² |
| \$4\pi\$ | Geometrical factor from spherical symmetry | — | Arises from integration over a sphere |
The electric field produced by a point charge in free space follows the inverse‑square law:
\$\boxed{E = \dfrac{Q}{4\pi\varepsilon_0 r^{2}}}\$
Remember to keep track of units, square the distance, and assign the correct radial direction based on the sign of \$Q\$. Mastery of this formula underpins many later topics, such as electric potential, field superposition, and electrostatic forces between multiple charges.