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An electric field is a region of space where a charged object experiences a force. We visualize fields using field lines: arrows that show the direction a positive test charge would be pushed. Lines emerge from positive charges and terminate on negative charges. Where lines are dense, the field is strong; where they're sparse, it's weak.

Coulomb's law describes the force between two point charges, and from it we derive the field strength E=kqr2E = \frac{kq}{r^2}. Electric potential (voltage) is related but different: it tells you the potential energy per unit charge at a point in the field. Equipotential lines (surfaces where voltage is constant) are always perpendicular to field lines.

Key Facts

  • Coulomb's Law: F=kq1q2r2F = \frac{kq_1q_2}{r^2} (k=8.99×109 Nm2/C2k = 8.99 \times 10^9 \text{ N}\cdot\text{m}^2/\text{C}^2)
  • Electric field strength: E=Fq=kqr2E = \frac{F}{q} = \frac{kq}{r^2} (units: N/C or V/m)
  • Field lines run from positive to negative charges.
  • Field lines never cross each other.
  • Between parallel plates, the field is uniform: E=VdE = \frac{V}{d}
  • Electric potential energy: U=qVU = qV (potential energy = charge ×\times voltage)

Vocabulary

Electric field (E)
Force per unit positive charge at a point in space; measured in N/C.
Field line
A line whose direction shows the direction of the electric force on a positive test charge.
Coulomb's Law
The force between two point charges is proportional to their charges and inversely proportional to the square of the distance between them.
Electric potential (V)
Electric potential energy per unit charge at a point, measured in volts.
Equipotential
A surface or line along which the electric potential is constant; always perpendicular to field lines.

Common Mistakes to Avoid

  • Confusing electric field (a vector, force per charge) with electric potential (a scalar, energy per charge). They are related but not the same thing.
  • Assuming field lines show the path a charge would travel. A positive charge accelerates along field lines only if released from rest; moving charges curve due to changing field directions.
  • Forgetting that field strength falls off as 1/r² for a point charge - doubling distance reduces the field to one-quarter.
  • Thinking work done moving along an equipotential surface is nonzero. No work is done along an equipotential because the potential doesn't change.

Practice Questions

  1. 1 Two charges of +2 μC and -2 μC are 0.1 m apart. Find the force between them.
  2. 2 What is the electric field strength 0.3 m from a +5 μC point charge?
  3. 3 Sketch the field line pattern for two equal positive charges placed 4 cm apart.