MODULE 06 · E1 / UNIT 1 · ELECTROSTATICS

Electric Charge and Coulomb’s Law

Like charges repel, unlike charges attract, and the force falls off with the square of the distance.

Algebra core · calculus option

POINT CHARGES ON A PLANE · DRAG OR USE THE ARROW KEYS

The plane

Ready
Selectedq₁
Position (x, y)– m
Net force |F|– N
Fx– N
Fy– N
Direction– °

Model

Point charges at rest on a 1.0 m × 0.6 m plane, in vacuum. Each arrow is the electric force on the charge it starts from. F₁₂ means the force on q₁ due to q₂. Arrow lengths are proportional to force (scale bar, top right); press Rescale arrows after big changes.

Force graph

LIVE

The curve is F = k|q₁q₂|/r² for q₁ and q₂. The dot is the present distance; the hollow dot is the previous one.

Net force on each charge
Charge|F| (N)FxFy

Key ideas

ALGEBRA
Charge is quantizedq = n e,  e = 1.602 × 10⁻¹⁹ C
Coulomb’s lawF = k |q₁q₂| / r²
Coulomb constantk = 8.988 × 10⁹ N·m²/C²
SuperpositionFnet = F₁₂ + F₁₃ + … (vectors)

Like charges repel and unlike charges attract. The forces between two charges are a Newton’s third law pair: equal in size and opposite in direction, even when one charge is much bigger. With several charges, add the pair forces as vectors, component by component.

Show the calculus

Turn on for Coulomb’s law in vector form and the force from a charged rod, found by integrating over the charge.

Charging: friction, contact and induction

ELECTROSCOPE
How is it charged?
The rod

    Rod0
    Electroscope0
    Ground0
    Total0

    Each + or − symbol stands for a very large number of elementary charges (about 10⁹ e). Only electrons move; the positive charges stay fixed in the atoms. The total never changes: charging moves charge, it does not create it.

    SI units, k = 8.988 × 10⁹ N·m²/C². Charges are points held at rest; forces are computed exactly from Coulomb’s law and added as vectors. Charges cannot be placed closer than 4 cm.