Electric charge: Difference between revisions

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== Charge density ==
For a thin, long conductor (e.g., electric cable):
$$\text{charge density } \lambda = \frac{dQ}{dL}$$
For a thin surface (e.g., aluminium foil):
$$\text{charge density } \sigma = \frac{dQ}{dA}$$

Latest revision as of 06:33, 2 October 2026

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Electrical charge is a fundamental property of matter.

SI Unit

The SI unit of electrical charge is Coulomb (C), named after French physicist Charles Augustine de Coulomb.[1]

Charge of subatomic particles

Particle Symbol Absolute charge (Coulombs) Relative charge (to proton)
proton $p^+$ $+1.602 \times 10^{-19}$ +1
neutron $n^0$ 0 0
electron $e^-$ $-1.602 \times 10^{-19}$ −1

[2][3]

Properties

Quantisation

Any electrical charge is a whole multiple of $e \equiv 1.602 \cdot 10^{-19} C$.[1]

i.e.,

$$ \forall Q, Q=ae, a \in Z $$

Restricted type

A charge must be either positive or negative.[1]

Positive and negative charges can cancel each out, therefore the total charge of a system is the algebraic sum of charges of all its elements.[1]

i.e., $$ Q_{system}=\sum Q_{element} $$

Warning: This does not mean the entire system can be always approximated as a point charge of $\sum Q_{elements}$, as the distribution of charges heavily influence the electrostatic behaviour of a system.

Conservation

Charge can neither be created or destroyed but only transfered. The amount of charge in any closed system is constant.[1]

i.e.,

$$\sum Q = C$$

where C is a constant for any closed system.

Electrostatic force

Any charge exert an electrostatic force on any other charge.[1]

This phenomenon is described by Coulomb's law:

$$\vec F_{e}(B \to A)=-\frac{1}{4\pi \epsilon_0}\frac{Q_AQ_B}{\left\| AB \right\|^2}\widehat{AB}$$

where $A$,$B$ are point charges

Charge density

For a thin, long conductor (e.g., electric cable):

$$\text{charge density } \lambda = \frac{dQ}{dL}$$

For a thin surface (e.g., aluminium foil):

$$\text{charge density } \sigma = \frac{dQ}{dA}$$