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Quantisation of Charge

All observable charges are integer multiples of the elementary charge e. Fractional charges (quarks) are confined and never observed freely.
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Derivation

Statement

Every observable charge in nature is an integer multiple of the elementary charge ee:

q=ne,nZ,e=1.6022×1019 C\boxed{q = ne, \quad n \in \mathbb{Z}, \quad e = 1.6022 \times 10^{-19} \text{ C}}

Basis

Charge quantisation is not derived from more fundamental laws within classical electrostatics — it is an experimental fact, originally established by Millikan's oil drop experiment (1909–1913).

The proton carries charge +e+e, the electron e-e. All macroscopic charges arise from the transfer or accumulation of electrons (or, in ionised matter, protons).

Quarks

Quarks carry fractional charges (±e/3\pm e/3, ±2e/3\pm 2e/3), but they are permanently confined inside hadrons by the strong force. No fractionally charged object has ever been isolated. At the level of observable particles, quantisation in units of ee holds without exception.

Practical implication

For macroscopic charges (say 1μC6×10121\,\mu\text{C} \approx 6 \times 10^{12} electrons), nn is enormous and the discreteness is imperceptible. The continuum approximation used in Gauss's law and Coulomb's law is entirely valid.

Note
Charge quantisation has a deep connection to magnetic monopoles: Dirac showed in 1931 that the mere existence of a single magnetic monopole anywhere in the universe would force electric charge to be quantised.