\(I_d=V_0\,\omega Csin\omega t\)
\(I_d=V_0\,\omega Ccos\omega t\)
\(I_d=\frac{V_0}{\omega C}cos\omega t\)
\(I_d=\frac{V_0}{\omega C}sin\omega t\)
To determine the displacement current \(I_d\) for a capacitor connected to an AC voltage source, we start by examining the given voltage expression: \(V = V_0 \sin \omega t\), where:
In an AC circuit, the relationship between current and voltage in a capacitor is different from that in a resistor. For a capacitor, the current (or displacement current in this case) leads the voltage by a phase angle of \(\frac{\pi}{2}\) radians.
The displacement current through the capacitor is given by:
Now, differentiate the voltage \(V = V_0\sin\omega t\) with respect to time:
Substitute into the expression for current:
Simplifying, we get:
Thus, the displacement current is given by the expression: \(I_d = V_0 \omega C \cos \omega t\). This matches the provided correct answer.
The other options can be ruled out since they do not incorporate the correct behavior of current leading the voltage by \(\frac{\pi}{2}\) radians, as seen in the use of \(\cos\) instead of \(\sin\) for current.
Therefore, the correct option is:
A current-carrying coil is placed in an external uniform magnetic field. The coil is free to turn in the magnetic field. What is the net force acting on the coil? Obtain the orientation of the coil in stable equilibrium. Show that in this orientation the flux of the total field (field produced by the loop + external field) through the coil is maximum.
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The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.
Displacement current is a quantity appearing in Maxwell’s equations. Displacement current definition is defined in terms of the rate of change of the electric displacement field (D). It can be explained by the phenomenon observed in a capacitor.
