The magnetic flux, through a circular coil of resistance R, changes by an amount Δϕ in a time Δt. Then the total quantity of electric charge ‘Q’, that passes any point in the coil, during the time Δt, is represented by
(1) \(Q=\frac{1}{R}\frac{Δϕ}{dt}\)
(2) \(Q=\frac{Δϕ}{R}\)
(3) \(Q=\frac{RΔϕ}{dt}\)
(4) \(Q=-\frac{Δϕ}{R}\)