Current, Resistance, and DC Circuits

Current, voltage, and resistance

A current is a flow of charge: \(I = \dfrac{dQ}{dt}\), measured in amperes ¹. It is driven around a circuit by a potential difference — a voltage \(V\) — supplied by a source such as a battery. How much current a given voltage drives through a component is set by its resistance \(R\), through Ohm’s law:

Resistance is measured in ohms (Ω); a larger \(R\) means less current for the same voltage. Components that obey this linear relation are called ohmic. The electrical power dissipated (as heat or work) follows from voltage and current ¹:

Series and parallel resistance

Real circuits combine many resistances, and two patterns cover most cases. The figure contrasts them.

In series, components lie on a single path, so the same current flows through each, and the resistances simply add ¹:

In parallel, components share the same two nodes, so each sees the same voltage, while the current splits among them. The reciprocals add:

so the equivalent resistance is always less than the smallest branch — adding parallel paths makes it easier for current to flow.

Kirchhoff’s laws

Series and parallel rules are shortcuts for the two general principles that govern any circuit, Kirchhoff’s laws ¹:

• Current law (KCL): the currents entering a node equal the currents leaving it — charge is conserved.
• Voltage law (KVL): around any closed loop, the voltage rises and drops sum to zero — energy is conserved.

Applied together, these laws turn a circuit into a system of linear equations in the unknown currents or node voltages — precisely the \(A\mathbf x = \mathbf b\) problem from the linear-algebra lessons. That connection, and analysis of circuits that store energy (capacitors and inductors) and respond over time, is where the Electrical track’s Circuit Analysis course picks up.