1.

Derivesigma=("ne"^2 tau)/m, where the symbols have their usual meaning.

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Solution :Let .n. be the numberdensityof electrons , .L. be the lengthof the CONDUCTORA and .A.be the areaof cross -sectionof the conductor .
Let `v_d` be the drift VELOCITYOF the electrons and Dx be a small length .
Electrons drift in a directionoppositeto the electric field. Number ofelectronsin .Dx.and area of cross -section .A.is equal to (ADx) n.
Charge on the theseelectrons =(nADx)e.
If Dt is the time taken for effectivedisplacementof electronsthen rate of flow charge = `nAe ((Deltax)/(Deltat))` .
By DEFINITION,electric current I=rate of flowof charge
i.e.,`I=nAev_d`...(1)
where , average velocityof electrons with whichit drifts againstthe directionof electric field is known as drift velocity`(v_d)`.
Let .a. be the accelerationof electrons. Let .E.be the electricfieldintensity . Force on electrons,
F=ma
i.e., eE=ma
But = `a=v_dt` where .t.is the relaxationtime .
Relaxationtime representsthe average timetaken for two successivecollisionsof electronsand ionsin the lattice.

Hence ,`eE=mv_dt` or `v_d=(eE)/(mtau)` ...(2)
We alsoknow that electricpotentialdifferencebetween the ends of the conductorV=EL
`v_d =(eV)/(mtauL)` substitutingthis is the expression (1)
We write, `I=nAe ((eV)/(mtauL))`
i.e., `I=((nAe^2)/(mtauL))V`
`R=(mtau L)/(nAe^2)`is called the electricalresistanceof a conductor . and `K=((nAe^2)/(mtauL))` is called the electric conductance of a conductor . the expression `sigma =("NE"^2)/(mtau)` is called the electricalconductivityand `1/sigma=(mtau)/("ne"^2)` is called electricalresistivity .


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