Alternating Current Class 12 NCERT Solutions: Important Topics, Questions And Free PDF

7.1 Resistance of the resistor, R = 100 Ω

Supply voltage, V = 220 V

Supply frequency,  $\nu$ = 50 Hz

The rms value of current is given as, I = $\frac{V}{R}$ = $\frac{220}{100}$ = 2.2 A

The net power consumed over a full cycle is given as P = VI = 220 $\times 2.2$ = 484 W

7.2 Peak voltage of the AC supply,  $V_o$ = 300 V

RMS voltage is given by $V_{rms}$ = $\frac{\mathrm{}{V}_o}{\surd 2}$ = $\frac{\mathrm{}300}{\surd 2}$ = 212.13 V

The rms value of current, I = 10 A

Peak current $I_o$ = $\sqrt[]{2}I$ = $\sqrt[]{2}\times 10=14.1A$

7.3 Inductance of the Inductor, L = 44 mH = 44 $\times {10}^{-3}$ H

Supply voltage, V = 220 V

Supply frequency,  $\nu$ = 50 Hz

Angular frequency,  $\omega$ = 2 $\pi \nu$

Inductive reactance,  $X_L$ = $\omega L$ = 2 $\pi \nu L$

rms value of current is given as

I = $\frac{V}{X_L}$ = $\frac{220}{2\pi \times 50\times 44\mathrm{}\times {10}^{-3}}$ = 15.92 A

Hence, the rms value of the current in the circuit is 15.92 A.

7.4 Capacitance of the capacitor, C = 60 $\mu F$ = 60 $\times {10}^{-6}$ F

Supply voltage, V = 110 V

Supply frequency,  $\nu$ = 60 Hz

Angular frequency,  $\omega$ = 2 $\pi \nu$

Capacitive reactance,  $X_c$ = $\frac{1}{\omega C}$ = $\frac{1}{2\pi \nu C}$

rms value of current is given by I = $\frac{V}{X_c}$ = 110 $\times 2\times \pi \times 60\times$ 60 $\times {10}^{-6}$ = 2.49 A

Hence, the rms value of current is 2.49 A.

7.5 In the inductive circuit:

rms value of current, I = 15.92 A

rms value of voltage, V = 220 V

The net power absorbed can be obtained by

P = VI cos $\varnothing$ , where $\varnothing$ is the phase difference between alternating voltage and current = 90 $°$

So P = VI cos $90°$ = 0

In the capacitive circuit:

rms value of current, I = 2.49 A

rms value of voltage, V = 110 V

The net power absorbed can be obtained by

P = VI cos $\varnothing$ , where $\varnothing$ is the phase difference between alternating voltage and current = 90 $°$

So P = VI cos $90°$ = 0

7.6 Inductance, L = 2.0 H

Capacitance, C = 32 $\mu F$ = 32 $\times {10}^{-6}$ F

Resistance, R = 10 Ω

Resonant frequency is given by the relation,

${\omega }_r$ = $\frac{1}{\sqrt[]{LC}}$ = $\frac{1}{\sqrt[]{2\times 32\mathrm{}\times {10}^{-6}}}$ = 125 rad /s

Now Q value of the circuit is given as

Q = $\frac{1}{R}\sqrt[]{\frac{L}{C}}$ = $\frac{1}{10}\sqrt[]{\frac{2}{32\mathrm{}\times {10}^{-6}}}$ = 25

7.7 Capacitance of the capacitor, C = 30 $\mu F$ = 30 $\times {10}^{-6}$ F

Inductance of the Inductor, L = 27 mH = 27 $\times {10}^{-3}$ H

Angular frequency is given as

${\omega }_r$ = $\frac{1}{\sqrt[]{LC}}$ = $\frac{1}{\sqrt[]{27\mathrm{}\times {10}^{-3}\times 30\mathrm{}\times {10}^{-6}}}$ = 1.11 ${10}^3$ rad /s

7.8 Capacitance of the capacitor, C = 30$\mu F$ = 30$\times {10}^{-6}$ F

Inductance of the Inductor, L = 27 mH = 27$\times {10}^{-3}$ H

Charge on the capacitor, Q = 6 mC= 6$\times {10}^{-3}$ C

Total energy stored in the capacitor can be calculated as:

E =$\frac{1}{2}\frac{Q^2}{C}$ =$\frac{1}{2}\frac{({6\mathrm{}\times {10}^{-3})}^2}{30\mathrm{}\times {10}^{-6}}$= 0.6 J

Total energy at a later time will remain same because energy is shared between the capacitor and the inductor.

7.9 Given values:

Resistance R = 20 Ω

Inductance, L = 1.5 H

Capacitance, C = 35 $\mu F$ = 35 $\times {10}^{-6}$ F

AC power supply, V = 200 V

Impedance of the circuit is given by the relation,

Z = $\sqrt[]{R^2+{\left(X_{L-}{X}_C\right)}^2}$ where $X_L$ = Inductive reactance and $X_C$ = Capacitive reactance

At resonance $X_L$ = $X_C$

Hence Z = R = 20 Ω

Current in the circuit, I = $\frac{V}{Z}$ = $\frac{200}{20}$ = 10 A

Hence, the average power transferred to the circuit in one complete cycle = VI = 200 $\times 10$= 2000 W

7.10 Lower tuning frequency, ${\nu }_1$ = 800 kHz = 800 $\times {10}^3$ Hz

Upper tuning frequency, ${\nu }_2$ = 1200 kHz = 1200 $\times {10}^3$ Hz

Effective inductance of the circuit, L = 200 $\mu H$ = 200 $\times {10}^{-6}$ H

Capacitance of variable capacitor for lower tuning frequency ( ${\nu }_1)$ is given as

$C_1$ = $\frac{1}{{\omega }_1^{2}L}$ , where ${\omega }_1$ is the angular frequency for capacitor $C_1$ = 2 $\pi {\nu }_1$

Hence, ${\omega }_1$ = 2 $\pi \times$ 800 $\times {10}^3$ = 5.026 $\times {10}^6$ rad/s

$C_1$ = $\frac{1}{{\omega }_1^{2}L}$ = $\frac{1}{{(5.026\times {10}^6)}^2\times 200\mathrm{}\times {10}^{-6}}$ F = 1.9789 $\times {10}^{-12}$ F = 197.89 pF

Capacitance of variable capacitor for lower tuning frequency ( ${\nu }_2)$ is given as

$C_2$ = $\frac{1}{{\omega }_2^{2}L}$ , where ${\omega }_2$ is the angular frequency for capacitor $C_2$ = 2 $\pi {\nu }_2$

Hence, ${\omega }_2$ = 2 $\pi \times$ 1200 $\times {10}^3$ = 7.54 $\times {10}^6$ rad/s

$C_1$ = $\frac{1}{{\omega }_2^{2}L}$ = $\frac{1}{{(7.54\times {10}^6)}^2\times 200\mathrm{}\times {10}^{-6}}$ F = 87.95 $\times {10}^{-12}$ F = 87.95 pF

Hence, the range of variable frequency is from 88 pF to 198 pF.

7.11 Inductance of the Inductor, L = 5.0 H

Resistance of the resistor, R = 40 Ω

Capacitance of the capacitor, C = 80 $\mu F=$ 80 $\times {10}^{-6}$ F

Potential of the voltage source, V = 230 V

Resonance angular frequency is given as

${\omega }_r$ = $\frac{1}{\sqrt[]{LC}}$ = $\frac{1}{\sqrt[]{5\times 80\mathrm{}\times {10}^{-6}}}$ = 50 rad/s

$\mathrm{H}\mathrm{e}\mathrm{n}\mathrm{c}\mathrm{e},\mathrm{}\mathrm{t}\mathrm{h}\mathrm{e}\mathrm{}\mathrm{c}\mathrm{i}\mathrm{r}\mathrm{c}\mathrm{u}\mathrm{i}\mathrm{t}\mathrm{}\mathrm{w}\mathrm{i}\mathrm{l}\mathrm{l}\mathrm{}\mathrm{c}\mathrm{o}\mathrm{m}\mathrm{e}\mathrm{}\mathrm{i}\mathrm{n}\mathrm{}\mathrm{r}\mathrm{e}\mathrm{s}\mathrm{o}\mathrm{n}\mathrm{a}\mathrm{n}\mathrm{c}\mathrm{e}\mathrm{}\mathrm{f}\mathrm{o}\mathrm{r}\mathrm{}\mathrm{a}\mathrm{}\mathrm{s}\mathrm{o}\mathrm{u}\mathrm{r}\mathrm{c}\mathrm{e}\mathrm{}\mathrm{f}\mathrm{r}\mathrm{e}\mathrm{q}\mathrm{u}\mathrm{e}\mathrm{n}\mathrm{c}\mathrm{y}\mathrm{}\mathrm{o}\mathrm{f}\mathrm{}50\mathrm{}\mathrm{r}\mathrm{a}\mathrm{d}/\mathrm{s}$

The impedance of the circuit is given as

Z = $\sqrt[]{R^2+{\left(X_{L-}{X}_C\right)}^2}$ where $X_L$ = Inductive reactance and $X_C$ = Capacitive reactance

At resonance, $X_L$ = $X_C$ so Z = R = 40Ω

Amplitude of the current at the resonating frequency is given as

$I_o$ = $\frac{V_0}{Z}$ where $V_0$ = Peak voltage = $\surd 2$ V

$I_o$ = $\frac{\surd 2\mathrm{V}}{Z}$ = $\frac{\surd 2\times 230}{40}$ = 8.13 A

Hence, at resonance, the impedance of the circuit is 40 Ω and the amplitude of the current is 8.13 A.

rms potential drop across the inductor is given by

${{(V}_l)}_{rms}$ = $I_{rms}$ $\times {\omega }_{r}L$

$I_{rms}=$ $\frac{I_o}{\surd 2}$ = $\frac{8.13}{\surd 2}$ = 5.75 A

$Hence,$ ${{(V}_l)}_{rms}$ = $5.75$ $\times 50\times 5$ = 1437.5 V

Potential drop across capacitor,

${{(V}_C)}_{rms}$ = $I_{rms}$ $\times \frac{1}{{\omega }_r\times C}$

$Hence,$ ${{(V}_l)}_{rms}$ = $5.75$ $\times \frac{1}{50\times 80\mathrm{}\times {10}^{-6}}$ = 1437.5 V

Potential drop across resistor,

${{(V}_R)}_{rms}$ = $I_{rms}$ $\times R$ = 5.75 $\times 40$ = 230 V

Potential drop across LC combination

${{(V}_{LC})}_{rms}$ = $I_{rms}$ $(X_L-X_C)$

At resonance, $X_L$ = $X_C)$ , hence

${{(V}_{LC})}_{rms}=0$

Hence, it is proved that the potential drop across the LC combination is zero at resonating frequency.

7.12 Inductance of the Inductor, L = 20 mH = 20 $\times$ ${10}^{-3}$ H

Capacitance of the capacitor, C = 50 $\mu F$ = 50 $\times {10}^{-6}$ F

Initial charge of the capacitor, Q = 10 mC = 10 $\times {10}^{-3}$ C

The total energy stored initially at the circuit is given as

E = $\frac{1}{2}$ $\times \frac{Q^2}{C}$ = $\frac{1}{2}$ $\times \frac{{(10\mathrm{}\times {10}^{-3})}^2}{50\mathrm{}\times {10}^{-6}}$ = 1 J

Hence, the total energy stored in the LC circuit will be conserved because there is no resistor connected in the circuit.

Natural frequency of the circuit is given by the relation

$\nu =\frac{1}{2\pi \sqrt[]{LC}}$ = $\frac{1}{2\pi \sqrt[]{20\times \mathrm{}{10}^{-3}\times 50\mathrm{}\times {10}^{-6}}}$ = 159.15 Hz

Natural angular frequency, $\omega =\frac{1}{\sqrt[]{LC}}$ = $\frac{1}{\sqrt[]{20\times \mathrm{}{10}^{-3}\times 50\mathrm{}\times {10}^{-6}}}$ = 1000 rad/s

(i) Total time period, T = $\frac{1}{\nu }$ = $\frac{1}{159.15}$ = 6.28 $\times {10}^{-3}$ s = 6.28 ms

Total charge on the capacitor at time t is given by

Q’ = Q $\cos ?\frac{2\pi }{T}$ t

For energy stored in electrical, we can write Q = Q’

Hence, it can be inferred that the energy stored in the capacitor is completely electrical at time, t = 0, $\frac{T}{2}$ , T , $\frac{3T}{2}$ , ……

(ii) Magnetic energy is the maximum when electrical energy Q’ s equal to zero.

Hence it can be inferred that the energy stored in the capacitor is completely magnetic at time, t = $\frac{T}{4},\frac{3T}{4},\frac{5T}{4}$ ……..

Let Q’ be the charge on the capacitor when total energy is equally shared between the capacitor and the inductor a time t. When total energy is equally shared between the inductor and capacitor, the energy stored in the capacitor = $\frac{1}{2}$ (maximum energy)

= $\frac{1}{2}\frac{{Q\text{'}}^2}{C}$ = $\frac{1}{2}$ ( $\frac{1}{2}\frac{Q^2}{C}$ ) = $\frac{1}{4}\frac{Q^2}{C}$

${Q\text{'}}^2$ = $\frac{Q^2}{2}$ or Q’ = $\frac{Q}{\surd 2}$

We have previously obtained Q’ = Q $\cos ?\frac{2\pi }{T}$ t

$\frac{Q}{\surd 2}=$ Q $\cos ?\frac{2\pi }{T}$ t

$\cos ?\frac{2\pi }{T}$ t = $\frac{1}{\surd 2}$ = cos(2 $n+1)\frac{\pi }{4}$ , where n = 0,1,2,3…….

t = (2n+1) $\frac{T}{8}$

Hence, total energy is equally shared between the inductor and the capacitor at time,

t = $\frac{T}{8}$ , $\frac{3T}{8}$ , $\frac{5T}{8}$ ,………

Resistor damps out the LC oscillations eventually. The whole of the initial energy (= 1.0 J) is eventually dissipated as heat.

7.13 Inductance of the Inductor, L = 0.50 H

Resistance of the resistor, R = 100 Ω

Potential of supply voltage, V = 240 V

Frequency of the supply, $\nu$ = 50 Hz

Peak voltage is given as $V_0$ = $\sqrt[]{2V}=\sqrt[]{2}\times 240$ = 339.41 V

Angular frequency of the supply, $\omega =2\pi \nu$ = 2 $\pi \times 50=314.16rad/s$

Maximum current in the supply is given as

$I_0$ = $\frac{V_0}{\sqrt[]{R^2+{\left(\omega L\right)}^2}}$ = $\frac{339.41}{\sqrt[]{{100}^2+{(314.16\times 0.50)}^2}}$ = 1.82 A

Equation for voltage is given as V = $V_0$ $\cos ?\omega t$ and equation for current is given as

I = $I_0\cos ?(\omega t-\varnothing )$ , where $\varnothing =$ phase difference between voltage and current.

At time t = 0, V = $V_0$ [Maximum voltage condition]

For $\omega t-\varnothing$ = 0, I = $I_0$ [ Maximum current condition], for that t = $\frac{\varnothing }{\omega }$

Hence the time lag between maximum voltage and maximum current is $\frac{\varnothing }{\omega }$

Phase angle is also given by the relation,

$\tan ?\varnothing$ = $\frac{\omega L}{R}$ = $\frac{314.16\times 0.5}{100}$ = 1.5708

$\varnothing =57.52°$

= $\frac{57.52\times \pi }{180}$ rad = 1.003 rad

$\omega t=1.003$

t = $\frac{1.003}{\omega }$ = $\frac{1.003}{314.16}$ = 3.20 $\times {10}^{-3}$ s = 3.2 ms

Hence the time lag between maximum voltage and maximum current is 3.2 ms.

7.14 Inductance of the Inductor, L = 0.50 H

Resistance of the resistor, R = 100 Ω

Potential of supply voltage, V = 240 V

Frequency of the supply, $\nu$ = 10 kHz = 10 $\times {10}^3$ Hz

Peak voltage is given as $V_0$ = $\sqrt[]{2V}=\sqrt[]{2}\times 240$ = 339.41 V

Angular frequency of the supply, $\omega =2\pi \nu$ = 2 $\pi \times {10}^{4}rad/s$

Maximum current in the supply is given as

$I_0$ = $\frac{V_0}{\sqrt[]{R^2+{\left(\omega L\right)}^2}}$ = $\frac{339.41}{\sqrt[]{{100}^2+{(2\pi \times {10}^4\times 0.50)}^2}}$ = 10.80 $\times {10}^{-3}$ A

Phase angle is also given by the relation,

$\tan ?\varnothing$ = $\frac{\omega L}{R}$ = $\frac{2\pi \times {10}^4\times 0.5}{100}$ = 314.16

$\varnothing =89.82°$

= $\frac{89.82\times \pi }{180}$ rad = 1.568 rad

$\omega t=1.568$

t = $\frac{1.568}{\omega }$ = $\frac{1.568}{2\pi \times {10}^4}$ = 24.95 $\times {10}^{-6}$ s = 24.95 $\mu$ s

It can be observed that $I_0$ is very small in this case. Hence, at high frequencies, the inductor amounts to an open circuit.

In a DC circuit, after a steady state is achieved, $\omega =0.$ Hence, inductor L behaves like a pure conducting object.

7.15 Capacitance of the capacitor, C = 100 $\mu F$ = 100 $\times {10}^{-6}$ F

Resistance of the resistor, R = 40 Ω

Supply voltage, V = 110 V

Frequency of the supply voltage, $\nu$ = 60 Hz

Angular frequency, $\omega$ = 2 $\pi \nu$ = 2 $\pi \times 60$ rad/s

For a RC circuit, the impedance Z, is given by Z = $\sqrt[]{R^2+\frac{1}{{\omega }^2{C}^2}}$

Z = $\sqrt[]{{40}^2+\frac{1}{{(2\pi \times 60)}^2{\times (100\times {10}^{-6})}^2}}$ = 47.996 Ω

Peak voltage, $V_0$ = $\surd 2\times V$ = $\surd 2\times 110$ = 155.56 V

Peak current, $I_0$ = $\frac{V_0}{Z}$ = $\frac{155.56\mathrm{}}{47.996}$ = 3.24 A

In a capacitor circuit, the voltage lags behind the current by a phase angle of $\varnothing$ . This angle is given by the relation

$\tan ?\varnothing$ = $\frac{\frac{1}{\omega C}}{R}$ = $\frac{1}{\omega CR}$ = $\frac{1}{2\pi \times 60\mathrm{}\times 100\times {10}^{-6}\times 40}$ = 0.663

$\varnothing =33.55°=\frac{33.55°\times \pi }{180}$ rad

$\mathrm{T}\mathrm{i}\mathrm{m}\mathrm{e}\mathrm{}\mathrm{l}\mathrm{a}\mathrm{g},t=\frac{\varnothing }{\omega }$ = $\frac{\frac{33.55°\times \pi }{180}}{2\pi \times 60}$ = $\frac{33.55\times \pi }{2\pi \times 60\times 180}$ = 1.55 $\times {10}^{-3}$ s = 1.55 ms

Hence the time lag between maximum current and maximum voltage is 1.55 ms.

7.16 Capacitance of the capacitor, C = 100 $\mu F$ = 100 $\times {10}^{-6}$ F

Resistance of the resistor, R = 40 Ω

Supply voltage, V = 110 V

Frequency of the supply voltage, $\nu$ = 12 kHz = 12 $\times {10}^3$ Hz

Angular frequency, $\omega$ = 2 $\pi \nu$ = 2 $\pi \times 12\mathrm{}\times {10}^3$ rad/s = 24 $\pi \times {10}^3$ rad/s

For a RC circuit, the impedance Z, is given by Z = $\sqrt[]{R^2+\frac{1}{{\omega }^2{C}^2}}$

Z = $\sqrt[]{{40}^2+\frac{1}{{(24\pi \times {10}^3)}^2{\times (100\times {10}^{-6})}^2}}$ = 40 Ω

Peak voltage, $V_0$ = $\surd 2\times V$ = $\surd 2\times 110$ = 155.56 V

Peak current, $I_0$ = $\frac{V_0}{Z}$ = $\frac{155.56\mathrm{}}{40}$ = 3.8

9 A

In a capacitor circuit, the voltage lags behind the current by a phase angle of $\varnothing$ . This angle is given by the relation

$\tan ?\varnothing$ = $\frac{\frac{1}{\omega C}}{R}$ = $\frac{1}{\omega CR}$ = $\frac{1}{24\pi \times {10}^3\times 100\times {10}^{-6}\times 40}$ = 3.315 $\times$ ${10}^{-3}$

$\varnothing =0.19°=\frac{0.19°\times \pi }{180}$ rad

$\mathrm{T}\mathrm{i}\mathrm{m}\mathrm{e}\mathrm{}\mathrm{l}\mathrm{a}\mathrm{g},t=\frac{\varnothing }{\omega }$ = $\frac{\frac{0.19°\times \pi }{180}}{24\pi \times {10}^3}$ = $\frac{0.19\times \pi }{24\pi \times {10}^3\times 180}$ = 4.4 $\times {10}^{-8}$ s = 0.044 $\mu$ s

Hence, $\varnothing$ tends to become zero at high frequencies. At a high frequency, capacitor C acts as a conductor.

In DC circuit, after the steady state is achieved, $\omega$ = 0

Hence, capacitor C amounts to an open circuit.

7.17 Inductance of the Inductor, L = 5.0 H

Resistance of the resistor, R = 40 Ω

Capacitance of the capacitor, C = 80 $\mu F=$ 80 $\times {10}^{-6}$ F

Potential of the voltage source, V = 230 V

Impedance Z of the given parallel LCR circuit is given as

$\frac{1}{Z}$ = $\sqrt[]{\frac{1}{R^2}+{(\frac{1}{\omega L}-\omega C)}^2}$ where $\omega$ = angular frequency

At resonance $\frac{1}{\omega L}-\omega C$ = 0 or ${\omega }^2$ = $\frac{1}{LC}$

$\omega =\sqrt[]{\frac{1}{LC}}$ = $\frac{1}{\sqrt[]{5\times 80\mathrm{}\times {10}^{-6}}}$ = 50 rad/s

The magnitude of Z is the maximum at $\omega$ = 50 rad/s. As a result, total current is minimum.

rms current flowing through the Inductor L is given as,

$I_L$ = $\frac{V}{\omega L}$ = $\frac{230}{50\times 5}$ = 0.92 A

rms current flowing through the Capacitor C is given as,

$I_L$ = $\frac{V}{\frac{1}{\omega C}}$ = 230 $\times 50\times$ 80 $\times {10}^{-6}$ = 0.92 A

rms current flowing through resistor R is given as, $I_R$ = $\frac{V}{R}$ = $\frac{230}{40}$ = 5.75 A

7.18 Inductance, L = 80 mH = 80 $\times {10}^{-3}$ H

Capacitance, C = 60 $\mu F$ = 60 $\times {10}^{-6}$ F

Supply voltage, V = 230 V

Supply frequency, $\nu$ = 50 Hz

Peak voltage, $V_0$ = V $\surd 2$ = 325.27 V

Angular frequency, $\omega$ = 2 $\pi \nu$ = 2 $\pi \times \nu$ = 2 $\pi \times 50$ = 100 $\pi$ rad/s

Maximum current is given as:

$I_0$ = $\frac{V_0}{(\omega L-\frac{1}{\omega C})}$ = $\frac{325.27\mathrm{}}{(100\pi \times 80\mathrm{}\times {10}^{-3}-\frac{1}{100\pi \times 60\mathrm{}\times {10}^{-6}})}$ = $-$ 11.65 A

The negative sign is due to $\omega L$ $<\frac{1}{\omega C}$

Amplitude of maximum current $\left|I_0\right|$ = 11.65 A

rms value of the current, I = $\frac{I_0}{\surd 2}$ = $\frac{-11.65}{\surd 2}$ = -8.24 A

(i) Potential difference across inductor, $V_L$ = I $\times \omega L$ = 8.24 $\times 100\pi \times$ 80 $\times {10}^{-3}$ V = 207.09 V

(ii) Potential drop across capacitor, $V_C$ = I $\times \frac{1}{\omega C}$ = 8.24 $\times \frac{1}{100\pi \times 60\mathrm{}\times {10}^{-6}}$ = 437.14 V

Average power consumed by the inductor is zero as actual voltage leads the current by $\frac{\pi }{2}$

Average power consumed by the capacitor is zero as the voltage lags current by $\frac{\pi }{2}$

The total power absorbed ( average over one cycle) is zero.

7.19 Inductance, L = 80 mH = 80 $\times {10}^{-3}$ H

Capacitance, C = 60 $\mu F$ = 60 $\times {10}^{-6}$ F

Resistance of the resistor, R = 15 Ω

Supply voltage, V = 230 V

Supply frequency, $\nu$ = 50 Hz

Peak voltage, $V_0$ = V $\surd 2$ = 325.27 V

Angular frequency, $\omega$ = 2 $\pi \nu$ = 2 $\pi \times \nu$ = 2 $\pi \times 50$ = 100 $\pi$ rad/s

Since the elements are connected in series, the impedance is given by

Z = $\sqrt[]{R^2+({\omega L-\frac{1}{\omega C})}^2}$

= $\sqrt[]{{15}^2+({100\pi \times 80\mathrm{}\times {10}^{-3}-\frac{1}{100\pi \times 60\mathrm{}\times {10}^{-6}})}^2}$

= $\sqrt[]{225+({25.133-53.052)}^2}$

= 31.693 Ω

Current flowing in the circuit, I = $\frac{V}{Z}$ = $\frac{230}{31.693}$ = 7.26 A

Average power transferred to resistance is given as $P_R$ = $I^2$ R = ${\left(7.26\right)}^2\times 15$ = 789.97 W

Average power transferred to capacitor, $P_C$ = 0

Average power transferred to Inductor, $P_L$ = 0

Total power absorbed by the circuit = $P_R+P_C+P_L=789.97+0+0=789.97W$

7.20 Inductance, L = 0.12 H

Capacitance, C = 480 nF = 480 $\times {10}^{-9}$ F

Resistance, R = 23 Ω

Supply voltage, V = 230 V

Peak voltage is given as, $V_0$ = $\sqrt[]{2}\times 230$ = 325.27 V

Current flowing in the circuit is given by the relation,

$I_0=\frac{V_0}{\sqrt[]{R^2+({\omega L-\frac{1}{\omega C})}^2}}$ where $I_0$ = maximum at resonance

$\mathrm{A}\mathrm{t}\mathrm{}\mathrm{r}\mathrm{e}\mathrm{s}\mathrm{o}\mathrm{n}\mathrm{a}\mathrm{n}\mathrm{c}\mathrm{e}\mathrm{}\mathrm{w}\mathrm{e}\mathrm{}\mathrm{h}\mathrm{a}\mathrm{v}\mathrm{e}\mathrm{}{\omega }_R\mathrm{L}-\mathrm{}\frac{1}{{\mathrm{\omega }}_{\mathrm{R}}\mathrm{C}}=0$ , where ${\omega }_R$ = Resonance angular frequency.

Hence, ${\omega }_R$ = $\frac{1}{\sqrt[]{LC}}$ = $\frac{1}{\sqrt[]{0.12\times 480\mathrm{}\times {10}^{-9}}}$ = 4166.67 rad/s

Therefore, resonating frequency ${\nu }_R$ = $\frac{{\omega }_R}{2\pi }$ = 663.15 Hz

Maximum current ${I_0}_{max}$ = $\frac{V_0}{R}$ = $\frac{325.27\mathrm{}}{23}$ = 14.14 A

Maximum average power absorbed by the circuit is given as

${P_{avg}}_{max}$ = $\frac{1}{2}{{I_0}_{max}}^2$ R = $\frac{1}{2}\times {14.14\mathrm{}}^2\times 23$ = 2300 W

The power transferred to the circuit is half the power at resonant frequency

Frequencies at which power transferred is half = ${\omega }_R\pm$ Δ $\omega$ = 2 $\pi ({\nu }_R\pm \Delta \nu )$ where,

Δ $\omega =\frac{R}{2L}$ = $\frac{23}{2\times 0.12}$ = 95.83 rad/s

$\Delta \nu$ = $\frac{\mathrm{\Delta }\omega }{2\pi }$ = $\frac{95.83}{2\times \pi }$ = 15.25 Hz

Therefore ${\nu }_R\pm \Delta \nu$ = 663.15 $\pm$ 15.25 = 647.9 Hz and 678.4 Hz

Hence, at 647.9 Hz and 678.4 Hz frequencies, the power transferred is half.

At these frequencies, current amplitude can be given as:

I’ = $\frac{1}{\surd 2}\times {I_0}_{max}$ = $\frac{14.14\mathrm{}}{\surd 2}$ = 10 A

Q factor of the given circuit can be obtained using the relation,

Q = $\frac{{\omega }_{R}L}{R}$ = $\frac{4166.67\times 0.12}{23}$ = 21.74

7.21 Given values of the LCR circuit

L = 3.0 H, C = 27 $\mu F=27\times {10}^{-6}$ F, R = 7.4 Ω

At resonance, the angular frequency,  ${\omega }_R$ = $\frac{1}{\sqrt[]{LC}}$ = $\frac{1}{\sqrt[]{3\times 27\times {10}^{-6}}}$ = 111.11 rad/s

Q factor of the series, Q = $\frac{{\omega }_R\mathrm{}\mathrm{L}}{R}$ = $\frac{111.11\times 3}{7.4}$ = 45.045

To improve the sharpness of the resonance by reducing its ‘full width at half maximum’ by a factor of 2 without changing ${\omega }_R$ , we need to reduce R to half i.e. R = $\frac{7.4}{2}$ = 3.7 Ω

7.22 (a) It is true that in any AC circuit, the applied voltage is equal to the average sum of instantaneous voltages across the series elements of the circuit. However, this is not true for rms voltages because voltage across different elements may not be in phase.

(b) A capacitor is used in the primary circuit of an induction coil. This is because when the circuit is broken, a high induced voltage is used to charge the capacitor to avoid sparks.

(c) The dc signal will appear across capacitor C because for dc signals, the impedance of an inductor (L) is negligible while the impedance of a capacitor © is very high (almost infinite). Hence, a dc signal appears across C

For an AC signal of high frequency, the impedance of L is high and that of C is very low. Hence, an AC signal of high frequency appears across L.

(d) If an iron core is inserted in the choke coil (which is in series with a lamp connected to AC line), then the lamp will glow dimly. This because the choke coil and the iron core increase the impedance of the circuit.

(e) A choke coil is needed in the use of fluorescent tubes with AC Mains because it reduces the voltage across the tube without wasting much power. An ordinary resistor cannot be used instead of choke coil for this purpose because it wastes power in the form of heat.

7.23 Input voltage,  $V_1$ = 2300 V

Number of turns in primary coil,  $n_1$ = 4000

Output voltage,  $V_2$ = 230 V

Number of turns in secondary coil = $n_2$

From the relation of voltage and number of turns, we get

$\frac{V_1}{V_2}$ = $\frac{n_1}{n_2}$ or $n_2=\frac{n_1{V}_2}{V_1}$ = $\frac{4000\times 230}{2300}$ = 400

Hence, there are 400 turns in the second winding.

7.24 Height of the water pressure head, h = 300 m

Volume of water flow rate, V = 100 $m^3$ /s

Efficiency of turbine generator,  $\eta$ = 60 % = 0.6

Acceleration due to gravity, g = 9.8 m/ $s^2$

Density of water,  $\rho$ = ${10}^3$ kg/ $m^3$

Therefore, electric power available from the plant = $\eta$ $\times h\rho gV$

= 0.6 $\times 300\times {10}^3\times 9.8\times 100$

= 176.4 $\times {10}^6$ W

= 176.4 MW

7.25 Total electric power required, P = 800 kW = 800 $\times {10}^3$ W

Supply voltage, V = 220 V

Electric plant generating voltage, V’ = 440 V

Distance between the town and power generating station, d = 15 km

Resistance of the two wires lines carrying power = 0.5 Ω /km

Total resistance of the wire, R = 2 $\times 15\times 0.5\Omega$ = 15 Ω

Step-down transformer rating 4000 – 220 V, hence

Input voltage to the transformer,  $V_1$ = 4000 V

Output voltage from the transformer,  $V_2$ = 220 V

rms current in the wire lines is given as

I = $\frac{P}{V_1}$ = $\frac{800\mathrm{}\times {10}^3}{4000}$ = 200 A

Line power loss = $I^{2}R$ = ${200}^2\times$ 15 = 600 $\times {10}^3$ W = 600 kW

Since the leakage power loss is negligible, the total power to be supplied by plat = 800 + 600 = 1400 kW

Voltage drop in the transmission line = IR = 200 $\times 15$ = 3000 V. Hence, the total voltage transmitted from plant = 3000 + 4000 = 7000 V

Since the power generated is 440V, the transformer rating at the plant should be 440 V – 7000 V

7.26 The rating of step-down transformer = 40000 V – 220 V

Hence, the input voltage,  $V_1$ = 40000 V

Output voltage,  $V_2$ = 220 V

Total electric power required, P = 800 kW = 800 $\times {10}^3$ W

Source potential, V = 220 V

Voltage at which electric plant generates power, V’ = 440 V

Distance between the town and power generating station, d = 15 km

Resistance of the two wires lines carrying power = 0.5 Ω /km

Total resistance of the wire, R = 2 $\times 15\times 0.5\Omega$ = 15 Ω

rms current in the wire lines is given as

I = $\frac{P}{V_1}$ = $\frac{800\mathrm{}\times {10}^3}{40000}$ = 20 A

Line power loss = $I^{2}R$ = ${20}^2\times$ 15 = 6 $\times {10}^3$ W = 6 kW

Since the leakage power loss is negligible, the total power to be supplied by plant = 800 + 6 = 806 kW

Voltage drop in the transmission line = IR = 20 $\times 15$ = 300 V. Hence, the total voltage transmitted from plant = 300 + 40000 = 40300 V

Since the power generated is 440V, the transformer rating at the plant should be 440 V – 40300 V

Hence, power loss during transmission = $\frac{6}{806}$ $\times 100$ = 0.744 %

In the previous exercise, power loss during transmission = $\frac{600}{1400}$ $\times 100$ = 42.86 %

Since the power loss is less for a high voltage transmission, high voltage transmission is preferred.