Coulomb's Law: The Field Around a Point Charge

1 · Predict

A single point charge sits alone in space. If you move a test point twice as far away, how much does the electric field strength drop?

2 · Set Up

  1. Open the single-charge preset and press Reset. The source charge is fixed at q = 5 nC.
  2. Enable the field-strength readout at a test point.
  3. Set the test point's distance from the charge for each trial and record the field strength.

3 · Collect Data

Distance r (m)Potential V (V)Field strength E (N/C)
1
2
3

Plot field strength E (y-axis) against 1/r² (x-axis) for your three trials. Is the line straight through the origin?

4 · Analyze

  1. For one trial, compute E = kq/r² using k = 8.99×10⁹ N·m²/C², q = 5 nC. Compare to the table.
  2. Explain, using the inverse-square law, why doubling the distance quarters the field strength rather than halving it.

5 · Extend

  1. Your potential column (V = kq/r) falls off more gently than the field (1/r instead of 1/r²). Explain why potential and field have different distance dependence even though both come from the same source charge.
  2. Coulomb's law E = kq/r² has the exact same mathematical form as Newton's gravitational field g = GM/r². Why might two completely different forces (electric and gravitational) share this inverse-square structure?

The Physics Behind This Experiment

Coulomb's Law

A point charge creates a radial electric field that falls off with the square of distance: E = kq/r², where k = 1/(4πε₀) ≈ 8.99×10⁹ N·m²/C². The force on a test charge is F = qE.

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