Drude model

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Drude Model electrons (shown here in blue) constantly bounce between heavier, stationary crystal ions (shown in red).

The Drude model of electrical conduction was proposed in 1900^[1] ^[2] by Paul Drude to explain the transport properties of electrons in materials (especially metals). The model, which is an application of kinetic theory, assumes that the microscopic behavior of electrons in a solid may be treated classically and looks much like a pinball machine, with a sea of constantly jittering electrons bouncing and re-bouncing off heavier, relatively immobile positive ions.

The two most significant results of the Drude model are an electronic equation of motion,

$\frac{d}{dt}\mathbf{p}(t) = q\mathbf{E} - \frac{\mathbf{p}(t)}{\tau},$

and a linear relationship between current density $J$ and electric field $E$ ,

$\mathbf{J} = \left( \frac{n q^2 \tau}{m} \right) \mathbf{E}.$

Here $t$ is the time and $p$ , $q$ , $n$ and $m$ , and $τ$ are respectively an electron's momentum, charge, number density, mass, and mean free time between ionic collisions. The latter expression is particularly important because it explains in semi-quantitative terms why Ohm's Law, one of the most ubiquitous relationships in all of electromagnetism, should be true.^[3] ^[4] ^[5]

[edit] Explanations

[edit] DC field

The simplest analysis of the Drude model assumes that electric field $\mathbf{E}$ is both uniform and constant, and that the thermal velocity of electrons is sufficiently high such that they accumulate only an infinitesimal amount of momentum $d\mathbf{p}$ between collisions, which occur on average every $τ$ seconds.^[6]

Then an electron isolated at time $t$ will on average have been traveling for time $τ$ since its last collision, and consequently will have accumulated momentum

$d\langle\mathbf{p}\rangle = q \mathbf{E} \tau.$

During its last collision, this electron will have been just as likely to have bounced forward as backward, so all prior contributions to the electron's momentum may be ignored, resulting in the expression

$\langle\mathbf{p}\rangle = q \mathbf{E} \tau.$

Substituting the relations

$\langle\mathbf{p}\rangle = m \langle\mathbf{v}\rangle,$

$\mathbf{J} = n q \langle\mathbf{v}\rangle,$

results in the formulation of Ohm's Law mentioned above:

$\mathbf{J} = \left( \frac{n q^2 \tau}{m} \right) \mathbf{E}.$

[edit] Time-varying analysis

The dynamics may also be described by introducing an effective drag force. At time $t = t 0 + d t$ the average electron's momentum will be

$\langle\mathbf{p}(t_0+dt)\rangle=\left( 1 - \frac{dt}{\tau} \right) \left(\langle\mathbf{p}(t_0)\rangle + q\mathbf{E}dt + ... \right),$

because, on average, $(1 - d t / τ)$ electrons will not have experienced another collision, and the ones that have will contribute to the total momentum to only a negligible order. ^[7]

With a bit of algebra, this results in the differential equation

$\frac{d}{dt}\langle\mathbf{p}(t)\rangle = q\mathbf{E} - \frac{\langle\mathbf{p}(t)\rangle}{\tau},$

where $\langle\mathbf{p}\rangle$ denotes average momentum, m the effective mass and q the charge of the electrons. This, which is an inhomogeneous differential equation, may be solved to obtain the general solution of

$\langle\mathbf{p}(t)\rangle = q \tau \mathbf{E} + \mathbf{C} e^{-t/\tau}$

for p(t). The steady state solution ( $\frac{d}{d t}\langle\mathbf{p}\rangle = 0$ ) is then

$\langle\mathbf{p}\rangle = q \tau \mathbf{E},$

As above, average momentum may be related to average velocity and this in turn may be related to current density,

$\langle\mathbf{p}\rangle = m \langle\mathbf{v}\rangle,$

$\mathbf{J} = n q \langle\mathbf{v}\rangle,$

and the material can be shown to satisfy Ohm's Law with a DC-conductivity $\, \sigma_0$ :

$\mathbf{J} = \left( \frac{n q^2 \tau}{m} \right) \mathbf{E}.$

The Drude model can also predict the current as a response to a time-dependent electric field with an angular frequency $\, \omega$ , in which case

$\sigma(\omega) = \frac{\sigma_0}{1 + i\omega\tau}.$

Here it is assumed that

$E(t) = \Re(E_0 e^{i\omega t});$

$J(t) = \Re(\sigma(\omega) E_0 e^{i\omega t}).$

In other conventions, $\, i$ is replaced by $\, -i$ in all equations. The imaginary part indicates that the current lags behind the electrical field, which happens because the electrons need roughly a time $\, \tau$ to accelerate in response to a change in the electrical field. Here the Drude model is applied to electrons; it can be applied both to electrons and holes; i.e., positive charge carriers in semiconductors.

[edit] Accuracy of the model

This simple classical Drude model provides a very good explanation of DC and AC conductivity in metals, the Hall effect, and thermal conductivity (due to electrons) in metals. The model also explains the Wiedemann-Franz law of 1853. However, it greatly overestimates the electronic heat capacities of metals. In reality, metals and insulators have roughly the same heat capacity at room temperature. Although the model can be applied to positive (hole) charge carriers, as demonstrated by the Hall effect, it does not predict their existence.

One note of trivia surrounding the theory is that in his original paper Drude made a conceptual error, estimating electrical conductivity to in fact be only half of what it classically should have been.^[8]

[edit] See also

[edit] References

^ Drude, Paul (1900). "Zur Elektronentheorie der metalle". Annalen der Physik 306 (3): 566. http://www3.interscience.wiley.com/cgi-bin/fulltext/112485959/PDFSTART.
^ Drude, Paul (1900). "Zur Elektronentheorie der Metalle; II. Teil. Galvanomagnetische und thermomagnetische Effecte". Annalen der Physik 308 (11): 369. http://www3.interscience.wiley.com/cgi-bin/fulltext/112485893/PDFSTART.
^ Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 6–7. ISBN 0-03-083993-9.
^ Edward M. Purcell (1965). Electricity and Magnetism. McGraw-Hill. pp. 117–122. ISBN 978-0070049086.
^ David J. Griffiths (1999). Introduction to Electrodynamics. Prentice-Hall. pp. 289. ISBN 978-81-203-161-0.
^ Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 6–7. ISBN 0-03-083993-9.
^ Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 11. ISBN 0-03-083993-9.
^ Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 23. ISBN 0-03-083993-9.

[0] Drude, Paul (1900). "Zur Elektronentheorie der metalle". Annalen der Physik 306 (3): 566. http://www3.interscience.wiley.com/cgi-bin/fulltext/112485959/PDFSTART.

[1] Drude, Paul (1900). "Zur Elektronentheorie der Metalle; II. Teil. Galvanomagnetische und thermomagnetische Effecte". Annalen der Physik 308 (11): 369. http://www3.interscience.wiley.com/cgi-bin/fulltext/112485893/PDFSTART.

[2] Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 6–7. ISBN 0-03-083993-9.

[3] Edward M. Purcell (1965). Electricity and Magnetism. McGraw-Hill. pp. 117–122. ISBN 978-0070049086.

[4] David J. Griffiths (1999). Introduction to Electrodynamics. Prentice-Hall. pp. 289. ISBN 978-81-203-161-0.

[5] Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 6–7. ISBN 0-03-083993-9.

[6] Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 11. ISBN 0-03-083993-9.

[7] Neil W. Ashcroft; N. David Mermin (1976). Solid State Physics. Saunders College. pp. 23. ISBN 0-03-083993-9.

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Drude model

From Wikipedia, the free encyclopedia

Contents

[edit] Explanations

[edit] DC field

[edit] Time-varying analysis

[edit] Accuracy of the model

[edit] See also

[edit] References

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