quantity

electron number density

electron number density — from formula anatomy
7 related articles · 3 formulas

Description

Electron number density is the number of free electrons per unit volume in a material or plasma. It is a fundamental parameter in plasma physics, solid-state physics, and astrophysics, determining how a medium conducts electricity, reflects light, or supports electromagnetic waves. In metals, it is roughly the density of conduction electrons; in plasmas, it sets the plasma frequency above which the medium becomes transparent to radiation.

History

The concept was formalized in the early 20th century with the Drude model of metals (1900) and later in plasma physics, though the term 'electron density' became widespread with the development of ionospheric research in the 1920s.

How it works

The electron number density nₑ is typically measured in electrons per cubic meter (m⁻³) or per cubic centimeter (cm⁻³). It enters key formulas such as the plasma frequency ωₚ = √(nₑe²/ε₀mₑ), where e is the electron charge, ε₀ the vacuum permittivity, and mₑ the electron mass. In a metal, nₑ is on the order of 10²⁸ m⁻³, while in a laboratory plasma it might be 10¹⁶–10¹⁹ m⁻³, and in the interstellar medium as low as 10⁴–10⁶ m⁻³.

In practice

Electron number density is used to design semiconductor devices, to interpret plasma etching and fusion experiments, and to calibrate ionospheric radio propagation models.

Fun fact

In the Earth's ionosphere, the electron number density peaks around 300 km altitude at about 10¹² m⁻³, which is why long-distance radio communication relies on that layer reflecting signals.

Concept graph →

Formulas

$$\mathrm{DM} = \int n_e \, dl$$
Integrated electron density along the line of sight.
What is in the formula
DMvariableDispersion measure — dispersion measure parsec per cubic centimetre
n_evariableElectron number density — electron number density per cubic metre
lvariablePath length along line of sight — length metre
∫operatorIntegration along the line of sight — integral
$$\text{RM} = \frac{e^3}{2\pi m_e^2 c^4} \int n_e B_\parallel \, dl$$
Rotation measure is proportional to the integral of electron density times parallel magnetic field along the line of sight.
What is in the formula
n_evariableelectron number density — electron number density per cubic metre
B_parallelvariablemagnetic field component along line of sight — magnetic flux density tesla
dlvariableinfinitesimal path element along line of sight metre
econstantelementary charge — elementary charge = 1.602176634e-19 coulomb
m_econstantelectron rest mass — electron mass = 9.1093837015e-31 kilogram
cconstantspeed of light in vacuum — speed of light = 299792458 metre per second
∫operatorsummation over the line of sight — integral operator
$$\text{DM} = \int_0^z n_e(z') \, \frac{c \, dz'}{H(z')}$$
Dispersion measure is the integral of electron density over redshift-dependent path length.
What is in the formula
n_e(z')variableelectron number density at redshift z' — electron number density per cubic metre
zvariablesource redshift — redshift
z'variableintegration variable redshift — redshift
cconstantspeed of light in vacuum — speed of light = 299792458 metre per second
∫operatorsummation over redshift from 0 to z — integral operator

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