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In fig, a square loop consistaing of an ...

In fig, a square loop consistaing of an inductor of inductance L and resistor of resistance R is placed between two long parallel wires. The two long straight wires have time - varing current of magnitude `I=(I_0) cos omega t` but the direction of current in them are opposite

Magnitude of emf in this circuit only due to flux change associated with two long straight current carrying wires will be

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In fig, a square loop consistaing of an inductor of inductance L and resistor of resistance R is placed between two long parallel wires. The two long straight wires have time - varing current of magnitude I=(I_0) cos omega t but the direction of current in them are opposite Total magnetic flux in this loop is

In fig, a square loop consistaing of an inductor of inductance L and resistor of resistance R is placed between two long parallel wires. The two long straight wires have time - varing current of magnitude I=(I_0) cos omega t but the direction of current in them are opposite Total magnetic flux in this loop is

In fig, a square loop consistaing of an inductor of inductance L and resistor of resistance R is placed between two long parallel wires. The two long straight wires have time - varing current of magnitude I=(I_0) cos omega t but the direction of current in them are opposite. The instantaneous current in the circuit will be

The field due to a long straight wire carrying a current I is proportional to

The field due to a long straight wire carrying a current I is proportional to …..

The magnetic induction at any point due to a long straight wire carrying a current is

A square loop of side 'a' with a capacitor of capacitance C is located between two current carrying long parallel wires as shown. The value of I in the wires in given as I=(I_0) sin omega t . (a) Calculate maximum current in the square loop. (b) Draw a graph between charges on the upper plates of the capacitor vs time.