Learning objectives
- Relate field strength and potential in uniform fields.
- Use inverse-square behavior for point-charge field predictions.
- Reason about direction and sign conventions for electric fields.
Interactive practice
Focus: Move the probe deliberately and explain trend changes before checking the displayed values.
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Change one variable, save another reading, then compare the evidence.
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Move the probe deliberately and explain trend changes before checking the displayed values.
E = F/q and E = −dV/dr. For a point charge, E = kQ/r² and V = kQ/r; between ideal parallel plates, E ≈ ΔV/d.
The probe is a negligible positive test charge. Point charges are idealized and edge effects are ignored in the central parallel-plate model.
Electric potential is a scalar; electric field is a vector. Zero potential does not necessarily mean zero field.
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