Think of an electric field as a force map that surrounds a charged object.
If you place a tiny test charge (like a small ball) in this map, the field tells the ball how to move.
It’s invisible, but its effect is real—just like the wind pushes a kite even though you can’t see the air molecules.
The electric field strength produced by a point charge in free space is:
\$E = \frac{Q}{4\pi\epsilon_0 r^2}\$
A point charge of \$+2.0\,\mu\text{C}\$ is placed at the origin.
What is the electric field 0.10 m away?
\$E = \frac{2.0\times10^{-6}}{4\pi(8.85\times10^{-12})(0.10)^2}\$
\$E \approx \frac{2.0\times10^{-6}}{1.112\times10^{-12}} \approx 1.80\times10^{6}\,\text{N/C}\$
| Symbol | Value | Units |
|---|---|---|
| \$Q\$ | Any charge | Coulomb (C) |
| \$r\$ | Distance from charge | metre (m) |
| \$\epsilon_0\$ | \$8.854\times10^{-12}\$ | F/m |
• Always check the units—they must cancel to give N/C.
• Remember that \$E\$ points away from a positive charge and toward a negative one.
• For multiple charges, use the principle of superposition: add the vectors of each field.
• If the problem asks for the field at a point, identify the distance \$r\$ correctly; it’s not the distance between charges unless specified.
• Practice converting microcoulombs to coulombs and meters to centimeters to avoid mistakes.