Electric current is the rate at which electric charge flows past a given point in a circuit. It is defined by the relation
$$ I = \frac{\Delta Q}{\Delta t} $$where $I$ is the current (in amperes, A), $\Delta Q$ is the amount of charge that passes (in coulombs, C), and $\Delta t$ is the time interval (in seconds, s).
In conductive materials the charge is carried by particles known as charge carriers. The nature of these carriers depends on the material:
All observed charge carriers carry charge in integer multiples of a fundamental unit, the elementary charge $e$:
$$ q = n\,e \qquad n = \pm1,\pm2,\pm3,\dots $$The accepted value of the elementary charge is
$$ e = 1.602 \times 10^{-19}\ \text{C} $$This quantisation means that charge cannot exist in arbitrary fractions; it is always an integer multiple of $e$.
| Carrier | Symbol | Charge ($q$) | Typical Material |
|---|---|---|---|
| Electron | $e^{-}$ | $-e$ | Metals, semiconductors |
| Proton | $p^{+}$ | $+e$ | Atomic nuclei |
| Alpha particle | $\alpha^{2+}$ | $+2e$ | Radioactive decay |
| Sodium ion | $\text{Na}^{+}$ | $+e$ | Electrolytes |
| Chloride ion | $\text{Cl}^{-}$ | $-e$ | Electrolytes |
When a current $I$ flows through a conductor, the number of charge carriers $N$ passing a cross‑section per second is given by
$$ N = \frac{I}{e} $$For example, a current of $1\ \text{A}$ corresponds to
$$ N = \frac{1\ \text{C s}^{-1}}{1.602 \times 10^{-19}\ \text{C}} \approx 6.24 \times 10^{18}\ \text{carriers per second} $$