Electric Forces and Fields Cheat Sheet
The core ideas of Electric Forces and Fields distilled into a single, scannable reference — perfect for review or quick lookup.
Quick Reference
Coulomb's Law
The electrostatic force between two point charges is $F = k |q_1 q_2| / r^2$, where $k = 8.99 \times 10^9$ N m$^2$/C$^2$ is Coulomb's constant, $q_1$ and $q_2$ are the charges, and $r$ is the distance between them. Like charges repel; opposite charges attract.
Electric Field
A vector field that represents the force per unit positive test charge at every point in space: $\vec{E} = \vec{F}/q$. The electric field due to a point charge is $E = kq/r^2$, directed radially outward for positive charges and inward for negative charges.
Electric Field Lines
Imaginary lines used to visualize electric fields. They start on positive charges and end on negative charges (or extend to infinity). The density of lines at a point is proportional to the field strength, and the tangent to a line gives the field direction. Field lines never cross.
Superposition Principle
The net electric field at any point due to multiple charges is the vector sum of the individual fields from each charge. Similarly, the net force on a charge is the vector sum of forces from all other charges. This principle holds because electric fields obey linearity.
Electric Potential
The electric potential $V$ at a point is the electric potential energy per unit positive charge: $V = U/q = kQ/r$ for a point charge. It is a scalar quantity measured in volts (1 V = 1 J/C). Potential differences, not absolute potentials, are physically meaningful.
Electric Potential Energy
The energy stored in a system of charges due to their positions: $U = kq_1q_2/r$ for two point charges. Positive $U$ means repulsion (like charges); negative $U$ means attraction (opposite charges). This energy can be converted to kinetic energy as charges move.
Gauss's Law
The total electric flux through any closed surface equals the enclosed charge divided by the permittivity of free space: $\oint \vec{E} \cdot d\vec{A} = Q_{\text{enc}} / \epsilon_0$. This law is most useful when charge distributions have high symmetry (spherical, cylindrical, or planar).
Conductors in Electrostatic Equilibrium
In a conductor at electrostatic equilibrium: (1) the internal electric field is zero, (2) excess charge resides entirely on the surface, (3) the surface is an equipotential, and (4) the external field is perpendicular to the surface. These properties arise because free charges redistribute until no net force acts on them.
Insulators and Dielectrics
Materials in which charges are not free to move throughout the bulk. When placed in an electric field, the molecules in a dielectric polarize (positive and negative ends shift), reducing the internal field. The dielectric constant $\kappa$ quantifies this reduction: $E_{\text{inside}} = E_0 / \kappa$.
Key Terms at a Glance
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