Drift velocity

In physics, drift velocity is the average velocity attained by charged particles, such as electrons, in a material due to an electric field. In general, an electron in a conductor will propagate randomly at the Fermi velocity, resulting in an average velocity of zero. Applying an electric field adds to this random motion a small net flow in one direction; this is the drift.

Drift velocity of electrons

Drift velocity is proportional to current. In a resistive material, it is also proportional to the magnitude of an external electric field. Thus Ohm's law can be explained in terms of drift velocity. The law's most elementary expression is:

u=\mu E,

where $u$ is drift velocity, $μ$ is the material's electron mobility, and $E$ is the electric field. In the MKS system, drift velocity has units of m/s, electron mobility, m²/(V·s), and electric field, V/m.

When a potential difference is applied across a conductor, free electrons gain velocity in the direction, opposite to the electric field between successive collisions (and lose velocity when traveling in the direction of the field), thus acquiring a velocity component in that direction in addition to its random thermal velocity. As a result, there is a definite small drift velocity of electrons, which is superimposed on the random motion of free electrons. Due to this drift velocity, there is a net flow of electrons opposite to the direction of the field. The drift speed of electrons is generally in the order of 10^-3 meters per second whereas the thermal speed is on the order of 10⁶ meters per second.

Experimental measure

The formula for evaluating the drift velocity of charge carriers in a material of constant cross-sectional area is given by:^[1]

u={j \over nq},

where $u$ is the drift velocity of electrons, $j$ is the current density flowing through the material, $n$ is the charge-carrier number density, and $q$ is the charge on the charge-carrier.

This can also be written as:

j=nqu

But the current density and drift velocity, j and u, are in fact vectors, so this relationship is often written as:

\mathbf {J} =\rho \mathbf {u} \,

where

\rho =nq

is the charge density (SI unit: coulombs per cubic metre).

In terms of the basic properties of the right-cylindrical current-carrying metallic ohmic conductor, where the charge-carriers are electrons, this expression can be rewritten as:

u={m\;\sigma \Delta V \over \rho ef\ell },

where

$u$ is again the drift velocity of the electrons, in m⋅s⁻¹
$m$ is the molecular mass of the metal, in kg
$σ$ is the electric conductivity of the medium at the temperature considered, in S/m.
$Δ V$ is the voltage applied across the conductor, in V
$ρ$ is the density (mass per unit volume) of the conductor, in kg⋅m⁻³
$e$ is the elementary charge, in C
$f$ is the number of free electrons per atom
$ℓ$ is the length of the conductor, in m

Numerical example

Electricity is most commonly conducted through copper wires. Copper has a density of 8.94 g/cm³ and an atomic weight of 63.546 g/mol, so there are 140685.5 mol/m³. In one mole of any element, there are 6.022×10²³ atoms (the Avogadro number). Therefore, in 1 m³ of copper, there are about 8.5×10²⁸ atoms (6.022×10²³ × 140685.5 mol/m³). Copper has one free electron per atom, so $n$ is equal to 8.5×10²⁸ electrons per cubic metre.

Assume a current $I$ = 1 ampere, and a wire of 2 mm diameter (radius = 0.001 m). This wire has a cross sectional area $A$ of π × (0.001 m)² = 3.14×10⁻⁶ m² = 3.14 mm². The charge of one electron is $q$ = −1.6×10⁻¹⁹ C. The drift velocity therefore can be calculated:

{\begin{aligned}u&={I \over nAq}\\&={\frac {1{\text{C}}/{\text{s}}}{\left(8.5\times 10^{28}{\text{m}}^{-3}\right)\left(3.14\times 10^{-6}{\text{m}}^{2}\right)\left(1.6\times 10^{-19}{\text{C}}\right)}}\\&=2.3\times 10^{-5}{\text{m}}/{\text{s}}\end{aligned}}

Dimensional analysis:

u={\dfrac {\text{A}}{{\dfrac {\text{electron}}{{\text{m}}^{3}}}{\cdot }{\text{m}}^{2}\cdot {\dfrac {\text{C}}{\text{electron}}}}}={\dfrac {\dfrac {\text{C}}{\text{s}}}{{\dfrac {1}{\text{m}}}{\cdot }{\text{C}}}}={\dfrac {\text{m}}{\text{s}}}

Therefore, in this wire, the electrons are flowing at the rate of 23 μm/s. At 60 Hz alternating current, this means that, within half a cycle (1/120th sec.), on average the electrons drift less than 0.2 μm. In context, at one ampere around 3×10¹⁶ electrons will flow across the contact point twice per cycle. But out of around 1×10²² movable electrons per meter of wire, this is an insignificant fraction.

By comparison, the Fermi flow velocity of these electrons (which, at room temperature, can be thought of as their approximate velocity in the absence of electric current) is around 1570 km/s.^[2]

References

↑ Griffiths, David (1999). Introduction to Electrodynamics (3 ed.). Upper Saddle River, NJ: Prentice-Hall. p. 289. ISBN 9780138053260.
↑ http://hyperphysics.phy-astr.gsu.edu/hbase/electric/ohmmic.html Ohm's Law, Microscopic View, retrieved 2015-11-16

External links

Ohm's Law: Microscopic View at Hyperphysics

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[1] Griffiths, David (1999). Introduction to Electrodynamics (3 ed.). Upper Saddle River, NJ: Prentice-Hall. p. 289. ISBN 9780138053260.

[2] ttp://hyperphysics.phy-astr.gsu.edu/hbase/electric/ohmmic.html Ohm's Law, Microscopic View, retrieved 2015-11-16

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[2]

Experimental measure

Numerical example

See also

References

External links