RMS Value of Current in Sinusoidal AC
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Q. In the below figure, a square loop consisting 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-varying current of magnitude I=I0 cos ωt A but the directions of current in them are opposite.
Total magnetic flux in this loop is
Total magnetic flux in this loop is
- μ0aI0cos ωtπln 2
- 2μ0aI0cos ωtπln 2
- 4μ0aI0cos ωtπln 2
- μ0aI0cos ωt2πln 2
Q. In the below figure, a square loop consisting 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-varying current of magnitude I=I0 cos ωt A, but the directions 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
- μ0a ln 2I0ωπsin ωt
- 2μ0a ln 2I0ωπsin ωt
- μ0a ln 2I0ω2πcos ωt
- μ0a ln 2I0ωπcos ωt
Q. Determine the rms value of a semi-circular current wave which has a maximum value of a Ampere. The y axis denotes current in Ampere and x axis denotes time.
- (1√2)a
- √32a
- √23a
- √13a
Q. If an alternating voltage is represented as E = 141 sin (628 t), then the rms value of the voltage and the frequency are respectively
- 141 V, 628 Hz
- 100 V, 50 Hz
- 100 V, 100 Hz
- 141 V, 100 Hz
Q. In a certain circuit current changes with time according to i=2√t.The r.m.s value of current between t = 2 to t = 4s will be
- 3A
- 3√3 A
- 2√3 A
- (2−√2) A