Coulomb force between two charges
How hard do two charges at this separation push, or pull, on each other?
- F
- Force, N
- q1
- First charge, C
- q2
- Second charge, C
- r
- Separation, m
LaTeX
F = k_e \frac{q1 \cdot q2}{r^2}
Result
F
Force
0.00036 N
Positive is repulsion (like charges), negative is attraction (opposite charges).
LaTeX
0.00036\,\mathrm{N} = k_e \frac{1\,\mathrm{nC} \cdot 1\,\mathrm{nC}}{5\,\mathrm{mm}^2}
This result is a link — the address bar holds your numbers, so it can be pasted into a post and opened to the same answer.
What this looks like
The formula behind the curve
- F
- Force, N
- q1
- First charge, C
- q2
- Second charge, C
- r
- Separation, m
LaTeX
F = k_e \frac{q1 \cdot q2}{r^2}
The formula behind the curve
- F
- Force, N
- q1
- First charge, C
- q2
- Second charge, C
- r
- Separation, m
LaTeX
F = k_e \frac{q1 \cdot q2}{r^2}
Method
- Convert both charges to coulombs and the separation to metres.
- Multiply the two charges together — same sign gives a positive product, opposite signs give a negative one.
- Divide by the square of the separation: the force falls off very fast with distance, a quarter as much again for every doubling.
- Multiply by Coulomb's constant, k_e = 8.9876×10⁹ N·m²/C². A positive result is a repulsive force pushing the charges apart; a negative result is attraction pulling them together.
Assumptions
- Both charges are treated as points, or as spheres small compared to the separation. Real particles with a finite size and a non-uniform charge distribution depart from this once they are close together.
- The medium between them is vacuum or air. A conductive or highly polar medium — water, for instance — screens the field and reduces the real force well below this figure.
- No other charges are present. In a real ionised gas stream a particle feels every other charge nearby, not just the one it is being compared against here.