Electric charge: Difference between revisions

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== Overview ==
'''Electrical charge''' is a fundamental property of matter.


fundamental physical property
== SI Unit ==
 
The SI unit of electrical charge is '''Coulomb (C)''', named after French physicist [[Person:Charles Augustine de Coulomb|Charles Augustine de Coulomb]].<ref>{{#cite:Q1934}}</ref>
 
== Charge of subatomic particles ==
 
{| class="wikitable"
! 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
|}
 
<ref>{{#cite:Q1791}}</ref><ref>{{#cite:Q1793}}</ref>
 
== Properties ==
 
=== Quantisation ===
 
Any electrical charge is a whole multiple of $e \equiv 1.602 \cdot 10^{-19} C$.<ref>{{#cite:Q1934}}</ref>
 
i.e.,
 
$$
\forall Q, Q=ae, a \in Z
$$
 
=== Restricted type ===
 
A charge must be either positive or negative.<ref>{{#cite:Q1934}}</ref>
 
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.<ref>{{#cite:Q1934}}</ref>
 
i.e.,
$$
Q_{system}=\sum Q_{element}
$$
 
<blockquote>
'''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.
</blockquote>
 
=== Conservation ===
 
Charge can neither be created or destroyed but only transfered. The amount of charge in any closed system is constant.<ref>{{#cite:Q1934}}</ref>
 
i.e.,
 
{{#content:Q1938}}
 
=== Electrostatic force ===
 
Any charge exert an electrostatic force on any other charge.<ref>{{#cite:Q1934}}</ref>
 
This phenomenon is described by Coulomb's law:
 
{{#content:Q1937}}
 
== 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):

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