Electrical properties of materials determine how they interact with electric charges and fields. Conductors allow charge to move easily, while insulators resist charge movement. These properties shape circuit design, electrical safety systems, and devices like capacitors.

Conductors vs. Insulators

The key difference between conductors and insulators comes down to how tightly a material holds onto its electrons.

Conductors have electrons that can move freely through the material. These "free electrons" aren't bound to any single atom, so when a voltage is applied, they flow easily as electric current. Common conductors include copper, aluminum, silver, and gold. You'll find them in electrical wiring, circuit boards, and lightning rods.

Insulators hold their electrons tightly in place, resisting the flow of charge. Materials like rubber, glass, plastic (PVC, Teflon, nylon), air, and wood are all insulators. They're used as coatings on electrical wires, as dielectrics in capacitors, and as protective barriers on high-voltage power lines.

The distinction isn't always absolute. Some materials (called semiconductors) fall between conductors and insulators, but that's a topic for later courses.

Why This Happens: Band Structure

Conductors and insulators also differ in their electronic band structure.

In conductors, the highest energy level occupied by electrons (called the Fermi level) sits within a partially filled energy band. Electrons can easily jump to nearby empty energy states, so they move freely.
In insulators, the Fermi level falls in a band gap, a range of energies where no electron states exist. Electrons would need a large energy boost to jump from the filled valence band to the empty conduction band, so current doesn't flow under normal conditions.

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Methods of Charging Objects

There are three main ways to give an object a net electric charge: friction, conduction, and induction.

Friction (triboelectric charging) transfers electrons when two objects are rubbed together. One material pulls electrons away from the other. For example, rubbing a balloon on your hair strips electrons from the hair onto the balloon. The balloon becomes negatively charged, and your hair becomes positively charged.

Conduction transfers charge through direct contact. When a charged object touches a neutral one, charge flows between them until they reach the same potential. If you touch a positively charged metal rod to a neutral metal sphere, electrons flow from the sphere to the rod, leaving the sphere positively charged.

Induction redistributes charge without direct contact. Bringing a negatively charged rod near a neutral metal sphere pushes electrons in the sphere away from the rod. The near side of the sphere becomes positive, and the far side becomes negative. If you then ground the far side (connect it to the earth), the excess electrons drain away, and the sphere is left with a net positive charge even after the rod is removed.

With induction, the charged object never touches the neutral one. That's the key difference from conduction.

Electric Force and Polarization

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Coulomb's Law

The electric force between two point charges follows Coulomb's law:

$F_e = k \frac{|q_1 q_2|}{r^2}$

where:

$F_e$ is the magnitude of the electric force
$q_1$ and $q_2$ are the two charges
$r$ is the distance between them
$k$ is Coulomb's constant: $k = 8.99 \times 10^9 \; \frac{N \cdot m^2}{C^2}$

Two things to notice about this equation:

Inverse square relationship: If you double the distance between two charges, the force drops to one-quarter of its original value. The force weakens rapidly with distance.
Sign matters for direction: Like charges (both positive or both negative) repel each other. Opposite charges attract. The absolute value bars in the formula give you the magnitude; you determine the direction from the signs of the charges.

Polarization in Insulators

Even though charges in an insulator can't flow freely, they can still shift slightly in response to an external electric field. This process is called polarization.

Here's what happens at the atomic level:

An external electric field is applied to the insulator.
The electron clouds around each atom shift slightly toward the positive side of the field, while the positive nuclei shift slightly toward the negative side.
Each atom becomes a tiny electric dipole (a pair of slightly separated positive and negative charges).
These dipoles create an internal electric field that opposes the external field.

The result is that the net electric field inside the insulator is weaker than the external field. How much weaker depends on the material's dielectric constant, a number that describes how easily the material polarizes.

Polarization has practical applications:

Capacitors place a dielectric (insulating) material between their plates. Polarization of the dielectric allows the capacitor to store more charge at the same voltage than it could with empty space between the plates.
Electrostatic shielding uses polarized insulators to reduce electric fields in a region, protecting sensitive electronic components.