>[!summary]
> The electric force is the force exerted by a charged particle
>
>
**Key equations:**
>
Force by a charged particle:
$F = \frac{q q_2}{4\pi R^2 \epsilon _0}$
>[!info]+ Read Time
**⏱ 2 mins**
# Definition
The electric force is the force experienced by a charged particle due to another charged particle or by an [[Electric Fields|electric field]].
The electric force can be defined in two ways, by [[Coulomb's Law|Coulomb's law]], where you define the force by a charged particle. Or by the electric field, where you define the force due to an electric field.
$
\begin{array}{c}
\text{Coulomb's Law:} \\
\vec{F} = \frac{\vec{q_{1}} \vec{q_{2}}}{4\pi R^2 \epsilon _0} \\
\\
\text{By the electric field:} \\
\vec{F}=q \vec{E}
\end{array}
$
# Deriving The Electric Force
>[!warning] Assumptions
Assume that a point charge will be in an electric field so that [[Forces]] are true
>
Also, assume the following:
> - The [[Electric Fields| electric field]] is defined as $F = q_1E$
> - From [[Coulomb's Law]] the electric force by a point charge is $E = \frac{q}{4\pi R^2 \epsilon _0}$
![[el_2.png]]
[^2]
>[!note] Explanation
A point charge in an electric field.
$\begin{array}{c}
\text{A point charge is in an electric field, the force on the point charge is equal to} \\
F = q_1E \\
\\
\text{From Coulombs Law we know:} \\
E = \frac{q_2}{4\pi R^2 \epsilon _0} \\
\\
\vec{F} = q(\frac{q_2}{4\pi R^2 \epsilon _0}) \\
\vec{F} = \frac{\vec{q_{1}} \vec{q_{2}}}{4\pi R^2 \epsilon _0}
\end{array}$
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[^1]: Taken from https://tikz.net/charge/ by Izaak Neutelings (July 2018)
[^2]: Taken from https://tikz.net/electric_field/ by Izaak Neutelings (July 2018)