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The magnetic flux ϕ , through a stationary loop of wire, having a resistance R, varies with time as ϕ = (at2 + bt) where a and b are positive constants. The average emf, and the total charge flowing in the loop in the time interval t = 0 to t = \(\tau\) , would be equal, respectively, to

(1) \((a\tau +b),(\frac{a\tau ^2+b \tau}{R})\)

(2) \((a\tau +b),(\frac{a\tau ^2+b \tau}{2R})\)

(3) \((\frac{a\tau +b}{2}),(\frac{a\tau ^2+b \tau}{R})\)

(4) \(2(a\tau +b),(\frac{a\tau ^2+b \tau}{2R})\)

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