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Derive σ = \(\frac{ne^2\tau}{m}\) Where the symbols have their usual meaning.

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Consider conductor of length x, area of cross section A. 

Vd = drift speed of free electrons, in a time t, let all the electrons travel a distance x = Vd ∆t. 

Electric current I = Q /t = neAvd 

The acceleration acquired by the free electrons is given by a = \(\frac{-eE}{m}\)

where m = mass of the electron 

If τ = relaxation time then velocity 

vd\(\frac{-eE}{m}\tau\)

Current density J = \(\frac{1}{A}\), J = σE therefore

σ = \(\frac{ne^2\tau}{m}\)

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