91影视

An inductor's obstruction in the current flow is known as inductive reactance. By determining the reactance due to the oscillation frequency within an inductor, we can get the current value by substituting this value in the voltage equation of Ohm's law.

The inductive reactance of a capacitor,

$X_L=2{\mathrm{蟺蹿}}_{\mathrm{d}}\mathrm{L}$...... (i)

The voltage equation from Ohm鈥檚 law,

$i_L=\frac{{}_{{鈭�}_m}}{X_L}$........ (ii)

Here, $f_d$is the driving frequency of oscillations, $L$is the inductance of the inductor, and ${鈭�}_m$is the emf applied across the circuit.

Since the circuit contains only the inductor and sinusoidal generator, the potential difference across the inductor and sinusoidal generator are the same.

$V_L={鈭�}_m$

${鈭�}_m$is the amplitude of the sinusoidal generator.

Thus, substituting equation (ii) in equation (i), we can get the resulting current through the inductor for frequency$f=1.00\mathrm{kHz}$ as follows:

$$\begin{gathered} I_L=\frac{{鈭�}_m}{2{\mathrm{蟺蹿}}_{\mathrm{d}}\mathrm{L}} \\ {I}_L=\frac{30\mathrm{V}}{2\mathrm{蟺}\left(1脳{10}^3\mathrm{Hz}\right)\left(50脳{10}^{-3}\mathrm{H}\right)} \\ {I}_L=0.0955\mathrm{A} \\ {I}_L=95.5\mathrm{mA} \end{gathered}$$

Hence, the value of current is $95.5\mathrm{mA}$.

The amplitude of alternating current if the frequency of emf is$8\mathrm{kHz}$.

In this case, the frequency is eight times larger than part a). Thus, the value of the resulting current is given as:

$$\begin{gathered} I_L=\frac{1}{8}\left(\frac{{鈭�}_m}{2{\mathrm{蟺蹿}}_{\mathrm{d}}\mathrm{L}}\right) \\ {I}_L=\frac{95.5\mathrm{mA}}{8} \\ {I}_L=11.9\mathrm{mA} \end{gathered}$$

Hence, the value of the current is $11.9\mathrm{mA}$.