Summary

General Principles

Coulomb’s Law

The forces between two charged particles q1 and q2 separated by distance r are

F1 on 2=F2 on 1=K|q1||q2|r2

The forces are repulsive for two like charges, attractive for two opposite charges.

The figure illustrates the forces between two positive charges labeled 1 and 2 kept a distance r from each other.

To solve electrostatic force problems:

Model Model objects as point charges.

Visualize Draw a picture showing charges and force vectors.

Solve Use Coulomb’s law and the vector addition of forces.

Review Is the result reasonable?

Important Concepts

The Charge Model

There are two kinds of charge, positive and negative.

  • Fundamental charges are protons and electrons, with charge ±e where e=1.60×10−19 C.

  • Objects are charged by adding or removing electrons.

  • The amount of charge is q=(Np−Ne)e.

  • An object with an equal number of protons and electrons is neutral, meaning no net charge.

Charged objects exert electric forces on each other.

  • Like charges repel, opposite charges attract.

  • The force increases as the charge increases.

  • The force decreases as the distance increases.

The figure consists of two parts that illustrate the forces between two different combinations of charges.

There are two types of material, insulators and conductors.

  • Charge remains fixed in or on an insulator.

  • Charge moves easily through or along conductors.

  • Charge is transferred by contact between objects.

Charged objects attract neutral objects.

  • Charge polarizes metal by shifting the electron sea.

  • Charge polarizes atoms, creating electric dipoles.

  • The polarization force is always an attractive force.

The figure illustrates the atoms in an insulator polarized by an external charge.

The Field Model

Charges interact with each other via the electric field E⃗.

  • Charge A alters the space around it by creating an electric field.

    The figure illustrates  the force exerted by an electric field on a charge labeled B by a charge labeled “A”.
  • The field is the agent that exerts a force. The force on charge qB is F⃗on B=qBE⃗.

An electric field is identified and measured in terms of the force on a probe charge q:

E⃗=F⃗on q/q
  • The electric field exists at all points in space.

  • An electric field vector shows the field only at one point, the point at the tail of the vector.

The electric field of a point charge is

E⃗=14πϵ0qr2 r^

Unit vector r^ indicates “away from q.”

The figure consists of two parts that illustrate the electric fields due to positive and negative charges.

Terms and Notation