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Formulas/physics/Electric Charges Fields/Superposition of Forces

Superposition of Forces

Net force on a charge q due to n other charges is the vector sum of individual Coulomb forces. Each pair interacts independently.
Class 11Class 12
Derivation

The principle

The superposition principle is an empirical fact: the force on a charge qq due to a collection of charges q1,q2,,qnq_1, q_2, \ldots, q_n is the vector sum of the individual Coulomb forces. The presence of other charges does not alter the interaction between any given pair.

Derivation

Let charge qq be at position r\vec{r}, and charge qiq_i at position ri\vec{r}_i. Define ri=rri\vec{r}_{i} = \vec{r} - \vec{r}_i as the vector from qiq_i to qq, with ri=rrir_i = |\vec{r} - \vec{r}_i|.

Force on qq due to qiq_i alone:

Fi=14πε0qqiri2r^i\vec{F}_i = \frac{1}{4\pi\varepsilon_0}\frac{q\, q_i}{r_i^2}\hat{r}_i

By superposition, the net force:

F=i=1nFi=q4πε0i=1nqiri2r^i\vec{F} = \sum_{i=1}^{n} \vec{F}_i = \frac{q}{4\pi\varepsilon_0}\sum_{i=1}^{n} \frac{q_i}{r_i^2}\hat{r}_i F=kqi=1nqiri2r^i\boxed{\vec{F} = k q \sum_{i=1}^{n} \frac{q_i}{r_i^2}\hat{r}_i}

Continuous distribution

When charge is distributed continuously with volume density ρ(r)\rho(\vec{r}'):

F=q4πε0ρ(r)(rr)rr3dV\vec{F} = \frac{q}{4\pi\varepsilon_0}\int \frac{\rho(\vec{r}')(\vec{r}-\vec{r}')}{|\vec{r}-\vec{r}'|^3}dV'
Note
Superposition fails in nonlinear media. In vacuum and linear dielectrics, it holds exactly.