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<strong>www</strong>.<strong>GOALias</strong>.<strong>blogspot</strong>.<strong>com</strong>CurrentElectricity2neσ = τ(3.23)mWe thus see that a very simple picture of electrical conductionreproduces Ohm’s law. We have, of course, made assumptions that τand n are constants, independent of E. We shall, in the next section,discuss the limitations of Ohm’s law.Example 3.1 (a) Estimate the average drift speed of conductionelectrons in a copper wire of cross-sectional area 1.0 × 10 –7 m 2 carryinga current of 1.5 A. Assume that each copper atom contributes roughlyone conduction electron. The density of copper is 9.0 × 10 3 kg/m 3 ,and its atomic mass is 63.5 u. (b) Compare the drift speed obtainedabove with, (i) thermal speeds of copper atoms at ordinarytemperatures, (ii) speed of propagation of electric field along theconductor which causes the drift motion.Solution(a) The direction of drift velocity of conduction electrons is oppositeto the electric field direction, i.e., electrons drift in the directionof increasing potential. The drift speed v dis given by Eq. (3.18)v d= (I/neA)Now, e = 1.6 × 10 –19 C, A = 1.0 × 10 –7 m 2 , I = 1.5 A. The density ofconduction electrons, n is equal to the number of atoms per cubicmetre (assuming one conduction electron per Cu atom as isreasonable from its valence electron count of one). A cubic metreof copper has a mass of 9.0 × 10 3 kg. Since 6.0 × 10 23 copperatoms have a mass of 63.5 g,236.0 × 10n = × 9.0 × 1063.5= 8.5 × 10 28 m –3which gives,61.5v d=28 –19 –78.5 × 10 × 1.6 × 10 × 1.0 × 10= 1.1 × 10 –3 m s –1 = 1.1 mm s –1(b) (i) At a temperature T, the thermal speed* of a copper atom ofmass M is obtained from [ = (3/2) k BT ] and is thustypically of the order of kBT/M , where k Bis the Boltzmannconstant. For copper at 300 K, this is about 2 × 10 2 m/s. Thisfigure indicates the random vibrational speeds of copper atomsin a conductor. Note that the drift speed of electrons is muchsmaller, about 10 –5 times the typical thermal speed at ordinarytemperatures.(ii) An electric field travelling along the conductor has a speed ofan electromagnetic wave, namely equal to 3.0 × 10 8 m s –1(You will learn about this in Chapter 8). The drift speed is, in<strong>com</strong>parison, extremely small; smaller by a factor of 10 –11 .EXAMPLE 3.1* See Eq. (13.23) of Chapter 13 from Class XI book.99

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