Question

(a) The bulb is in series with a capacitor along with the a.c. mains. The bulb lights with some intensity. What happens to th
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Answer #1

Capacitive reactance is given by

X_{C}=\frac{1}{j\omega C}

Therefore, the total impedence of the series RC circuit is

Z=\sqrt{R^{2}+X^{2}_{C}}=\sqrt{R^{2}+\frac{1}{\omega^{2} C^{2}}}

The intensity of the bulb (B) is proportional to the heat generated in the bulb. If the voltage of the AC source is V, then you can write

B\propto I^{2}R\propto\left (\frac{V}{Z} \right )^{2}\times R

\therefore B\propto \frac{R}{\sqrt{R^{2}+\frac{1}{w^{2}C^{2}}}}

(a) (i) Doubling the capacitance means intensity will increase according to above equation.

(ii) Doubling the frequency means intensity will increase according to above equation.

(iii) When the voltage reaches a threshold value, a current flows through the bulb that dramatically reduces its resistance, and the capacitor (capacitance C and time constant \tau ) discharges through the bulb as if the battery and charging resistor were not there. Once discharged, the process will start again, with a flash period of \tau .

(b) The circuit current (I) can be expressed as for AC RC circuit

I=\frac{V}{Z}=\frac{V}{\sqrt{R^{2}+\frac{1}{\omega^{2} C^{2}}}}

Here, in your problem, R = 20 ohm, C = 30 \mu F = 30 x 10-6 F, I = 3 mA = 3 x 10-3 A = 0.003 A, V = 24 Volt. Therefore,

0.003=\frac{24}{\sqrt{20^{2}+\frac{1}{\omega^{2} (30\times 10^{-6})^{2}}}}

\therefore 20^{2}+\frac{1}{\omega^{2} (30\times 10^{-6})^{2}}=64\times 10^{6}

\therefore \omega = 4.16\ rad/s

\therefore f = 0.663\ Hz

(c) (i) The current vs frequency will look like (Frequency along X-axes and Current along Y-axes)

(ii) THe current and voltage variation of resistor will be same as the figure above with frequency, but the data value indicated in the Y-axes will change accordingly.

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