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<strong>www</strong>.<strong>GOALias</strong>.<strong>blogspot</strong>.<strong>com</strong>PhysicsThus, mechanical energy which was needed to move the arm PQ isconverted into electrical energy (the induced emf) and then to thermal energy.There is an interesting relationship between the charge flow throughthe circuit and the change in the magnetic flux. From Faraday’s law, wehave learnt that the magnitude of the induced emf is,ΔΦBε = Δ tHowever,ΔQε = Ir = r Δ tThus,ΔΦBΔ Q =rExample 6.8 Refer to Fig. 6.12(a). The arm PQ of the rectangularconductor is moved from x = 0, outwards. The uniform magnetic field isperpendicular to the plane and extends from x = 0 to x = b and is zerofor x > b. Only the arm PQ possesses substantial resistance r. Considerthe situation when the arm PQ is pulled outwards from x = 0 to x = 2b,and is then moved back to x = 0 with constant speed v. Obtain expressionsfor the flux, the induced emf, the force necessary to pull the arm and thepower dissipated as Joule heat. Sketch the variation of these quantitieswith distance.(a)FIGURE 6.12216EXAMPLE 6.8Solution Let us first consider the forward motion from x = 0 to x = 2bThe flux Φ Blinked with the circuit SPQR isΦB= Blx 0 ≤ x < b= Blb b ≤ x < 2bThe induced emf is,dΦBε =−dt=−Blv 0 ≤ x < b= 0 b ≤ x < 2b

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