The graphs given below depict the dependence | vedclass

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(C) The inductive reactance is given by $X_L = \omega L = 2 \pi f L$. This shows that $X_L \propto f$,which is a straight line passing through the ori

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$X_1$ is a capacitor and $X_2$ is an inductor

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(C) The inductive reactance is given by $X_L = \omega L = 2 \pi f L$. This shows that $X_L \propto f$,which is a straight line passing through the origin.The capacitive reactance is given by $X_C = \frac{1}{\omega C} = \frac{1}{2 \pi f C}$. This shows that $X_C \propto \frac{1}{f}$,which is a rectangular hyperbola.From the given graphs,$X_1$ follows the relation $X_1 \propto \frac{1}{f}$,so $X_1$ is a capacitor.$X_2$ follows the relation $X_2 \propto f$,so $X_2$ is an inductor.Therefore,$X_1$ is a capacitor and $X_2$ is an inductor.

The graphs given below depict the dependence of two reactive impedances $X_1$ and $X_2$ on the frequency of the alternating $e.m.f.$ applied individually to them. We can then say that

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