AP Physics C: E&M · Unit 1: Electric Charges, Fields & Gauss's Law
1.2 Electric Fields
Defining the Electric Field
An electric field is the force per unit charge at a point in space, created by a source charge. Formally, E = F/q. It's a vector field: at every point it has magnitude and direction, pointing away from positive charges and toward negative charges. A test charge placed in the field experiences a force F = qE.
Field from a Point Charge
For a point charge Q, the field at distance r is E = kQ/r², directed radially. This follows directly from Coulomb's law divided by the test charge. Fields from multiple charges obey superposition: add the vector contributions from each source charge to find the net field at a point.
Continuous Charge Distributions
For charge spread over a line, surface, or volume, the field is found by integrating contributions from infinitesimal charge elements dq: dE = k(dq)/r². Symmetry (like uniform rings or rods) often simplifies these integrals by canceling perpendicular components, leaving only the net field along an axis of symmetry.
Key terms
- Electric field (definition)
- Force per unit charge, E = F/q; a vector pointing away from positive charges and toward negative charges.
- Field of a point charge
- E = kQ/r², directed radially outward (positive Q) or inward (negative Q).
- Superposition principle
- The net electric field at a point is the vector sum of the fields due to each individual source charge.
- Field from continuous charge distribution
- Found by integrating dE = k(dq)/r² over the entire charge distribution.
- Test charge
- A small hypothetical charge used to measure the electric field without disturbing the source charges.
Try an AP-style question
A −2 μC charge feels a 0.04 N force pointing west. What is the electric field there?
- 20,000 N/C west
- 5 × 10⁻⁵ N/C west
- 0.08 N/C east
- 20,000 N/C east
Show the answer
D. E = F/q; negative charge → opposite direction.
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