Total Force on Point Charge from Multiple Point Charges
Theorem
Let $q_1, q_2, \ldots, q_n$ be point charges.
For all $i$ in $\set {1, 2, \ldots, n}$ where $i \ne j$, let $\mathbf F_{i j}$ denote the force exerted on $q_j$ by $q_i$.
For all $i$ in $\set {1, 2, \ldots, n}$, let $\mathbf F_i$ denote the force exerted on $q_i$ by the combined action of all the other point charges.
Then the electrostatic force $\mathbf F_i$ exerted on $q_i$ by the combined action of all the other point charges is given by:
\(\ds \mathbf F_i\) | \(=\) | \(\ds \sum_{\substack {1 \mathop \le j \mathop \le n \\ i \mathop \ne j} } \mathbf F_{j i}\) | ||||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le n \\ i \mathop \ne j} } \dfrac {q_i q_j} {r_{j i}^3} \mathbf r_{j i}\) |
where:
- the summation denotes the vector sum of $\mathbf F_{ji}$
- $\mathbf r_{ij}$ denotes the displacement from $q_i$ to $q_j$
- $r_{ij}$ denotes the distance between $q_i$ and $q_j$
- $\varepsilon_0$ denotes the vacuum permittivity.
Proof
The proof proceeds by induction.
For all $n \in \Z_{\ge 2}$, let $\map P n$ be the proposition:
- $\ds \mathbf F_i = \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le n \\ i \mathop \ne j} } \dfrac {q_i q_j} {r_{j i}^3} \mathbf r_{j i}$
$\map P 2$ is the case:
$\mathbf F_1 = \dfrac 1 {4 \pi \varepsilon_0} \dfrac {q_1 q_2} {r_{2 1}^3} \mathbf r_{2 1}$
which is Coulomb's Law of Electrostatics.
Thus $\map P 0$ is seen to hold.
Basis for the Induction
$\map P 3$ is the case:
- $\mathbf F_1 = \dfrac {q_2 q_1} {4 \pi \varepsilon_0 r_{2 1}^3} \mathbf r_{2 1} + \dfrac {q_3 q_1} {4 \pi \varepsilon_0 r_{3 1}^3} \mathbf r_{3 1}$
which is proved in Total Force on Point Charge from 2 Point Charges.
Thus $\map P 3$ is seen to hold.
This is the basis for the induction.
Induction Hypothesis
Now it needs to be shown that if $\map P k$ is true, where $k \ge 1$, then it logically follows that $\map P {k + 1}$ is true.
So this is the induction hypothesis:
- $\ds \mathbf F_i = \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le k \\ i \mathop \ne j} } \dfrac {q_i q_j} {r_{j i}^3} \mathbf r_{j i}$
from which it is to be shown that:
- $\ds \mathbf F_i = \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le {k + 1} \\ i \mathop \ne j} } \dfrac {q_i q_j} {r_{j i}^3} \mathbf r_{j i}$
Induction Step
This is the induction step:
\(\ds \mathbf F_i\) | \(=\) | \(\ds \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le k \\ i \mathop \ne j} } \dfrac {q_i q_j} {r_{j i}^3} \mathbf r_{j i} + \dfrac {q_i q_{k + 1} } {4 \pi \varepsilon_0 r_{\paren {k + 1} i}^3} \mathbf r_{\paren {k + 1} i}\) | Basis for the Induction | |||||||||||
\(\ds \) | \(=\) | \(\ds \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le {k + 1} \\ i \mathop \ne j} } \dfrac {q_i q_j} {r_{j i}^3} \mathbf r_{j i}\) | Definition of Summation |
So $\map P k \implies \map P {k + 1}$ and the result follows by the Principle of Mathematical Induction.
Therefore:
- $\forall n \in \Z_{\ge 2}: \ds \mathbf F_i = \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le n \\ i \mathop \ne j} } \dfrac {q_i q_j} {r_{j i}^3} \mathbf r_{j i}$
$\blacksquare$
Also presented as
This can also be presented as:
- $\ds \mathbf F_i = \dfrac 1 {4 \pi \varepsilon_0} \sum_{\substack {1 \mathop \le j \mathop \le n \\ i \mathop \ne j} } \dfrac {q_i q_j} {\size {\mathbf r_j - \mathbf r_i}^3} \paren {\mathbf r_j - \mathbf r_i}$
where $\mathbf r_i$ denotes the position vector of $q_i$ with respect to the origin of the coordinate system used as a frame of reference.
Sources
- 1990: I.S. Grant and W.R. Phillips: Electromagnetism (2nd ed.) ... (previous) ... (next): Chapter $1$: Force and energy in electrostatics: $1.1$ Electric Charge: $(1.3)$