Published by Patrick Mutisya · 14 days ago
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} \$