ROUTERA


Alternating Current

Class 12th Physics Chapter HOTs


Question 1:

Q: Derive the expression for the instantaneous power in an AC circuit.

Solution: The instantaneous power in an AC circuit is given by:

p(t)=v(t)i(t)p(t) = v(t) \cdot i(t)

For an AC voltage v(t)=Vmsin(ωt)v(t) = V_m \sin(\omega t) and current i(t)=Imsin(ωt+ϕ)i(t) = I_m \sin(\omega t + \phi) , the instantaneous power is:

p(t)=Vmsin(ωt)Imsin(ωt+ϕ)p(t) = V_m \sin(\omega t) \cdot I_m \sin(\omega t + \phi)

Using the trigonometric identity for sinAsinB\sin A \sin B :

p(t)=VmIm2[cos(ϕ)cos(2ωt+ϕ)]p(t) = \frac{V_m I_m}{2} [\cos(\phi) - \cos(2\omega t + \phi)]

Thus, the instantaneous power is:

p(t)=VmIm2[cos(ϕ)cos(2ωt+ϕ)]p(t) = \frac{V_m I_m}{2} [\cos(\phi) - \cos(2\omega t + \phi)]

This shows that the instantaneous power is a combination of a constant term and a time-varying term.


Question 2:

Q: An AC circuit has a resistance of 10Ω10 \, \Omega and an inductance of 0.2H0.2 \, \text{H} . If the frequency of the source is 50Hz50 \, \text{Hz} and the maximum voltage is 220V220 \, \text{V} , calculate the impedance of the circuit.

Solution: The inductive reactance is given by:

XL=2πfL=2π×50×0.2=62.83ΩX_L = 2 \pi f L = 2 \pi \times 50 \times 0.2 = 62.83 \, \Omega

The total impedance ZZ is given by:

Z=R2+XL2=102+62.832=100+3947.23=62.99ΩZ = \sqrt{R^2 + X_L^2} = \sqrt{10^2 + 62.83^2} = \sqrt{100 + 3947.23} = 62.99 \, \Omega

Thus, the impedance of the circuit is approximately 62.99Ω62.99 \, \Omega .


Question 3:

Q: Calculate the average power consumed in an AC circuit when the voltage is 220V220 \, \text{V} , current is 5A5 \, \text{A} , and the phase difference between the voltage and current is 6060^\circ .

Solution: The average power is given by:

Pavg=VrmsIrmscosϕP_{\text{avg}} = V_{\text{rms}} I_{\text{rms}} \cos \phi

Substitute the given values:

Pavg=220×5×cos60=220×5×12=550WP_{\text{avg}} = 220 \times 5 \times \cos 60^\circ = 220 \times 5 \times \frac{1}{2} = 550 \, \text{W}

Thus, the average power consumed is 550W550 \, \text{W} .


Question 4:

Q: In a series RLC circuit, if the resistance is 10Ω10 \, \Omega , the inductance is 2H2 \, \text{H} , and the capacitance is 0.01F0.01 \, \text{F} , calculate the resonant frequency of the circuit.

Solution: The resonant frequency f0f_0 is given by:

f0=12πLCf_0 = \frac{1}{2 \pi \sqrt{LC}}

Substitute the given values:

f0=12π2×0.01=12π×0.1414=1.13Hzf_0 = \frac{1}{2 \pi \sqrt{2 \times 0.01}} = \frac{1}{2 \pi \times 0.1414} = 1.13 \, \text{Hz}

Thus, the resonant frequency is 1.13Hz1.13 \, \text{Hz} .


Question 5:

Q: A 200-turn coil has an area of 0.05m20.05 \, \text{m}^2 and is placed in a magnetic field of strength 0.2T0.2 \, \text{T} . If the coil rotates in the field with an angular velocity of 100rad/s100 \, \text{rad/s} , calculate the maximum induced EMF in the coil.

Solution: The maximum induced EMF is given by:

EMFmax=NABω\text{EMF}_{\text{max}} = N A B \omega

Substitute the given values:

EMFmax=200×0.05×0.2×100=200V\text{EMF}_{\text{max}} = 200 \times 0.05 \times 0.2 \times 100 = 200 \, \text{V}

Thus, the maximum induced EMF is 200V200 \, \text{V} .


Question 6:

Q: In a series LCR circuit, the applied voltage is 220V220 \, \text{V} , the resistance is 10Ω10 \, \Omega , the inductance is 0.5H0.5 \, \text{H} , and the capacitance is 0.002F0.002 \, \text{F} . Calculate the current in the circuit at resonance.

Solution: At resonance, the inductive reactance and capacitive reactance cancel out, so the impedance of the circuit is simply the resistance RR . Thus, the current is:

I=VR=22010=22AI = \frac{V}{R} = \frac{220}{10} = 22 \, \text{A}

Thus, the current at resonance is 22A22 \, \text{A} .


Question 7:

Q: A capacitor of capacitance 100μF100 \, \mu\text{F} is connected in series with a resistor of 50Ω50 \, \Omega to an AC supply of frequency 60Hz60 \, \text{Hz} . Calculate the reactance of the capacitor.

Solution: The capacitive reactance is given by:

XC=12πfC=12π×60×100×106=26.53ΩX_C = \frac{1}{2 \pi f C} = \frac{1}{2 \pi \times 60 \times 100 \times 10^{-6}} = 26.53 \, \Omega

Thus, the capacitive reactance is 26.53Ω26.53 \, \Omega .


Question 8:

Q: A coil has a self-inductance of 5H5 \, \text{H} . If the current in the coil changes from 0A0 \, \text{A} to 2A2 \, \text{A} in 0.1s0.1 \, \text{s} , calculate the induced EMF.

Solution: The induced EMF is given by:

EMF=LΔIΔt\text{EMF} = - L \frac{\Delta I}{\Delta t}

Substitute the given values:

EMF=5×200.1=100V\text{EMF} = - 5 \times \frac{2 - 0}{0.1} = - 100 \, \text{V}

Thus, the induced EMF is 100V100 \, \text{V} .


Question 9:

Q: Derive the expression for the average power consumed in an RLC circuit.

Solution: The average power in an RLC circuit is given by:

Pavg=VrmsIrmscosϕP_{\text{avg}} = V_{\text{rms}} I_{\text{rms}} \cos \phi

where cosϕ\cos \phi is the power factor. The power factor is:

cosϕ=RZ\cos \phi = \frac{R}{Z}

Thus, the average power becomes:

Pavg=VrmsIrmsRZP_{\text{avg}} = V_{\text{rms}} I_{\text{rms}} \cdot \frac{R}{Z}

where ZZ is the impedance of the circuit.


Question 10:

Q: In a series LCR circuit, the voltage across the resistor is 100V100 \, \text{V} , the voltage across the inductor is 150V150 \, \text{V} , and the voltage across the capacitor is 50V50 \, \text{V} . Find the total voltage in the circuit.

Solution: The total voltage in a series LCR circuit is given by:

Vtotal=VR2+(VLVC)2V_{\text{total}} = \sqrt{V_R^2 + (V_L - V_C)^2}

Substitute the given values:

Vtotal=1002+(15050)2=1002+1002=20000=141.42VV_{\text{total}} = \sqrt{100^2 + (150 - 50)^2} = \sqrt{100^2 + 100^2} = \sqrt{20000} = 141.42 \, \text{V}

Thus, the total voltage in the circuit is 141.42V141.42 \, \text{V} .


Question 11:

Q: A 100-turn coil has a radius of 0.1m0.1 \, \text{m} and is rotating with an angular velocity of 50rad/s50 \, \text{rad/s} in a uniform magnetic field of strength 0.2T0.2 \, \text{T} . Calculate the maximum induced EMF in the coil.

Solution: The maximum induced EMF is given by:

EMFmax=NABω\text{EMF}_{\text{max}} = N A B \omega

where A=πr2A = \pi r^2 . Substituting the values:

A=π×(0.1)2=0.0314m2A = \pi \times (0.1)^2 = 0.0314 \, \text{m}^2 EMFmax=100×0.0314×0.2×50=31.4V\text{EMF}_{\text{max}} = 100 \times 0.0314 \times 0.2 \times 50 = 31.4 \, \text{V}

Thus, the maximum induced EMF is 31.4V31.4 \, \text{V} .


Question 12:

Q: A series LCR circuit has a resonance frequency of 50 Hz, a resistance of 20 Ω, and an inductance of 0.4 H. Calculate the value of the capacitance in the circuit.

Solution: The resonance frequency f0f_0 is given by:

f0=12πLCf_0 = \frac{1}{2 \pi \sqrt{LC}}

Rearranging to find CC :

C=1(2πf0)2LC = \frac{1}{(2 \pi f_0)^2 L}

Substitute the values:

C=1(2π×50)2×0.4=1(314.16)2×0.4=0.000255F=255μFC = \frac{1}{(2 \pi \times 50)^2 \times 0.4} = \frac{1}{(314.16)^2 \times 0.4} = 0.000255 \, \text{F} = 255 \, \mu\text{F}

Thus, the capacitance is 255μF255 \, \mu\text{F} .


Question 13:

Q: In an LCR circuit, the resonance occurs at a frequency of 100 Hz. If the capacitor is replaced by one having twice the capacitance, what will be the new resonance frequency?

Solution: The resonance frequency is given by:

f0=12πLCf_0 = \frac{1}{2 \pi \sqrt{LC}}

If the capacitance is doubled, the new frequency f1f_1 will be:

f1=12πL×2C=f02f_1 = \frac{1}{2 \pi \sqrt{L \times 2C}} = \frac{f_0}{\sqrt{2}}

Substitute the given value f0=100Hzf_0 = 100 \, \text{Hz} :

f1=1002=70.71Hzf_1 = \frac{100}{\sqrt{2}} = 70.71 \, \text{Hz}

Thus, the new resonance frequency is 70.71Hz70.71 \, \text{Hz} .


Question 14:

Q: A coil has an inductance of 2H2 \, \text{H} and carries a current of 3A3 \, \text{A} . Calculate the energy stored in the coil.

Solution: The energy stored in the coil is given by:

E=12LI2E = \frac{1}{2} L I^2

Substitute the values:

E=12×2×32=12×2×9=9JE = \frac{1}{2} \times 2 \times 3^2 = \frac{1}{2} \times 2 \times 9 = 9 \, \text{J}

Thus, the energy stored in the coil is 9J9 \, \text{J} .


Question 15:

Q: In an AC circuit, the voltage is 220V220 \, \text{V} , the current is 5A5 \, \text{A} , and the phase difference between them is 3030^\circ . Find the reactance of the circuit.

Solution: The impedance of the circuit is given by:

Z=VI=2205=44ΩZ = \frac{V}{I} = \frac{220}{5} = 44 \, \Omega

The phase difference ϕ=30\phi = 30^\circ , so:

Z=R2+X2Z = \sqrt{R^2 + X^2}

where XX is the reactance. Since cos30=RZ\cos 30^\circ = \frac{R}{Z} , we can find RR :

R=Zcos30=44×32=38.05ΩR = Z \cos 30^\circ = 44 \times \frac{\sqrt{3}}{2} = 38.05 \, \Omega

Thus, the reactance X=Z2R2=44238.052=26.6ΩX = \sqrt{Z^2 - R^2} = \sqrt{44^2 - 38.05^2} = 26.6 \, \Omega .

Thus, the reactance is 26.6Ω26.6 \, \Omega .


Question 16:

Q: A 1000-turn coil has a radius of 0.1m0.1 \, \text{m} and is rotating with an angular velocity of 60rad/s60 \, \text{rad/s} in a magnetic field of strength 0.5T0.5 \, \text{T} . Find the average induced EMF in the coil during one complete rotation.

Solution: The induced EMF is given by:

EMFavg=NABω(average)\text{EMF}_{\text{avg}} = N A B \omega \text{(average)}

where A=πr2=π×(0.1)2=0.0314m2A = \pi r^2 = \pi \times (0.1)^2 = 0.0314 \, \text{m}^2 .

Substituting the values:

EMFavg=1000×0.0314×0.5×60=942V\text{EMF}_{\text{avg}} = 1000 \times 0.0314 \times 0.5 \times 60 = 942 \, \text{V}

Thus, the average induced EMF is 942V942 \, \text{V} .


Question 17:

Q: In an LCR circuit, the inductive reactance XL=30ΩX_L = 30 \, \Omega and capacitive reactance XC=40ΩX_C = 40 \, \Omega . What is the impedance of the circuit?

Solution: The impedance ZZ in an LCR circuit is given by:

Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}

Here, XL=30ΩX_L = 30 \, \Omega and XC=40ΩX_C = 40 \, \Omega , so:

Z=R2+(3040)2=R2+100ΩZ = \sqrt{R^2 + (30 - 40)^2} = \sqrt{R^2 + 100} \, \Omega

Without the resistance value RR , we cannot calculate ZZ . Thus, the impedance depends on the value of RR .


Question 18:

Q: A 220 V AC source is connected across a purely capacitive circuit with a capacitance of 10μF10 \, \mu\text{F} . Calculate the current flowing through the circuit.

Solution: The capacitive reactance XCX_C is given by:

XC=12πfCX_C = \frac{1}{2 \pi f C}

For f=50Hzf = 50 \, \text{Hz} and C=10μF=10×106FC = 10 \, \mu\text{F} = 10 \times 10^{-6} \, \text{F} :

XC=12π×50×10×106=318.31ΩX_C = \frac{1}{2 \pi \times 50 \times 10 \times 10^{-6}} = 318.31 \, \Omega

The current II is given by:

I=VXC=220318.31=0.691AI = \frac{V}{X_C} = \frac{220}{318.31} = 0.691 \, \text{A}

Thus, the current flowing through the circuit is 0.691A0.691 \, \text{A} .


Question 19:

Q: An AC circuit has a frequency of 100 Hz. If the inductance is 0.2H0.2 \, \text{H} , calculate the inductive reactance.

Solution: The inductive reactance is given by:

XL=2πfLX_L = 2 \pi f L

Substituting the given values:

XL=2π×100×0.2=125.66ΩX_L = 2 \pi \times 100 \times 0.2 = 125.66 \, \Omega

Thus, the inductive reactance is 125.66Ω125.66 \, \Omega .


Question 20:

Q: A transformer steps up the voltage from 110 V to 220 V. If the primary coil has 500 turns, how many turns does the secondary coil have?

Solution: The voltage ratio in a transformer is given by:

VsVp=NsNp\frac{V_s}{V_p} = \frac{N_s}{N_p}

Substituting the given values:

220110=Ns500\frac{220}{110} = \frac{N_s}{500}

Thus:

Ns=1000turnsN_s = 1000 \, \text{turns}

Therefore, the number of turns in the secondary coil is 10001000 .


Question 21:

Q: Calculate the power factor of a series LCR circuit where the resistance is 20Ω20 \, \Omega , the inductive reactance is 30Ω30 \, \Omega , and the capacitive reactance is 40Ω40 \, \Omega .

Solution: The impedance ZZ is given by:

Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}

Substituting the values:

Z=202+(3040)2=400+100=500=22.36ΩZ = \sqrt{20^2 + (30 - 40)^2} = \sqrt{400 + 100} = \sqrt{500} = 22.36 \, \Omega

The power factor cosϕ\cos \phi is given by:

cosϕ=RZ=2022.36=0.894\cos \phi = \frac{R}{Z} = \frac{20}{22.36} = 0.894

Thus, the power factor is 0.8940.894 .


Question 22:

Q: A coil with 100 turns has a radius of 0.1m0.1 \, \text{m} and is placed in a magnetic field of strength 0.5T0.5 \, \text{T} . If the coil rotates at a frequency of 50 Hz, calculate the maximum induced EMF.

Solution: The maximum induced EMF is given by:

EMFmax=NABω\text{EMF}_{\text{max}} = N A B \omega

where A=πr2=π×(0.1)2=0.0314m2A = \pi r^2 = \pi \times (0.1)^2 = 0.0314 \, \text{m}^2 and ω=2πf=2π×50=314.16rad/s\omega = 2 \pi f = 2 \pi \times 50 = 314.16 \, \text{rad/s} .

Substituting the values:

EMFmax=100×0.0314×0.5×314.16=492.7V\text{EMF}_{\text{max}} = 100 \times 0.0314 \times 0.5 \times 314.16 = 492.7 \, \text{V}

Thus, the maximum induced EMF is 492.7V492.7 \, \text{V} .


Question 23:

Q: In a series LCR circuit, the inductive reactance is 50Ω50 \, \Omega , the capacitive reactance is 30Ω30 \, \Omega , and the resistance is 40Ω40 \, \Omega . What is the phase angle ϕ\phi ?

Solution: The phase angle is given by:

tanϕ=XLXCR\tan \phi = \frac{X_L - X_C}{R}

Substitute the given values:

tanϕ=503040=2040=0.5\tan \phi = \frac{50 - 30}{40} = \frac{20}{40} = 0.5

Thus:

ϕ=tan1(0.5)=26.57\phi = \tan^{-1} (0.5) = 26.57^\circ

Therefore, the phase angle is 26.5726.57^\circ .


Question 24:

Q: A capacitor of 5μF5 \, \mu\text{F} is connected to an AC source of 230V230 \, \text{V} . If the frequency of the source is 50 Hz, find the capacitive reactance and the current in the circuit.

Solution: The capacitive reactance is given by:

XC=12πfC=12π×50×5×106=636.6ΩX_C = \frac{1}{2 \pi f C} = \frac{1}{2 \pi \times 50 \times 5 \times 10^{-6}} = 636.6 \, \Omega

The current II is given by:

I=VXC=230636.6=0.362AI = \frac{V}{X_C} = \frac{230}{636.6} = 0.362 \, \text{A}

Thus, the current in the circuit is 0.362A0.362 \, \text{A} .


Question 25:

Q: The resonance frequency of a series LCR circuit is 100Hz100 \, \text{Hz} . If the inductance is 1H1 \, \text{H} , find the capacitance in the circuit.

Solution: The resonance frequency is given by:

f0=12πLCf_0 = \frac{1}{2 \pi \sqrt{LC}}

Rearranging for CC :

C=1(2πf0)2LC = \frac{1}{(2 \pi f_0)^2 L}

Substitute the values:

C=1(2π×100)2×1=0.000025F=25μFC = \frac{1}{(2 \pi \times 100)^2 \times 1} = 0.000025 \, \text{F} = 25 \, \mu\text{F}

Thus, the capacitance is 25μF25 \, \mu\text{F} .


Question 26:

Q: A transformer has a primary voltage of 110 V and a secondary voltage of 220 V. If the primary current is 2 A, calculate the secondary current.

Solution: The power in the primary coil is:

Pprimary=VpIpP_{\text{primary}} = V_p I_p

The power in the secondary coil is:

Psecondary=VsIsP_{\text{secondary}} = V_s I_s

Assuming an ideal transformer, Pprimary=PsecondaryP_{\text{primary}} = P_{\text{secondary}} , so:

VpIp=VsIsV_p I_p = V_s I_s

Rearrange to find IsI_s :

Is=VpIpVs=110×2220=1AI_s = \frac{V_p I_p}{V_s} = \frac{110 \times 2}{220} = 1 \, \text{A}

Thus, the secondary current is 1A1 \, \text{A} .


Question 27:

Q: In a series LCR circuit, the phase difference between the current and the voltage is 45 degrees. If the resistance is 20 Ω and the inductive reactance is 30 Ω, calculate the capacitive reactance.

Solution: The phase angle ϕ\phi is given by:

tanϕ=XLXCR\tan \phi = \frac{X_L - X_C}{R}

Substitute the given values:

tan45=30XC20\tan 45^\circ = \frac{30 - X_C}{20}

Since tan45=1\tan 45^\circ = 1 , we have:

1=30XC201 = \frac{30 - X_C}{20}

Thus:

30XC=20XC=10Ω30 - X_C = 20 \quad \Rightarrow \quad X_C = 10 \, \Omega

Therefore, the capacitive reactance is 10Ω10 \, \Omega .


Question 28:

Q: A series LCR circuit has a voltage of 240 V, resistance of 40 Ω, inductive reactance of 60 Ω, and capacitive reactance of 30 Ω. Calculate the current in the circuit.

Solution: The total impedance ZZ is given by:

Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}

Substitute the given values:

Z=402+(6030)2=1600+900=2500=50ΩZ = \sqrt{40^2 + (60 - 30)^2} = \sqrt{1600 + 900} = \sqrt{2500} = 50 \, \Omega

The current II is given by:

I=VZ=24050=4.8AI = \frac{V}{Z} = \frac{240}{50} = 4.8 \, \text{A}

Thus, the current in the circuit is 4.8A4.8 \, \text{A} .


Question 29:

Q: The primary coil of a transformer has 200 turns, and the secondary coil has 600 turns. If the primary voltage is 110 V, find the secondary voltage.

Solution: The voltage ratio in a transformer is:

VsVp=NsNp\frac{V_s}{V_p} = \frac{N_s}{N_p}

Substitute the values:

Vs110=600200\frac{V_s}{110} = \frac{600}{200}

Thus:

Vs=110×3=330VV_s = 110 \times 3 = 330 \, \text{V}

Therefore, the secondary voltage is 330V330 \, \text{V} .


Question 30:

Q: A series LCR circuit has a resistance of 10 Ω, an inductive reactance of 20 Ω, and a capacitive reactance of 10 Ω. Calculate the power consumed in the circuit.

Solution: The total impedance ZZ is given by:

Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}

Substitute the given values:

Z=102+(2010)2=100+100=200=14.14ΩZ = \sqrt{10^2 + (20 - 10)^2} = \sqrt{100 + 100} = \sqrt{200} = 14.14 \, \Omega

The power factor is:

cosϕ=RZ=1014.14=0.707\cos \phi = \frac{R}{Z} = \frac{10}{14.14} = 0.707

The power consumed is:

P=VrmsIrmscosϕP = V_{\text{rms}} I_{\text{rms}} \cos \phi

Since the values of VrmsV_{\text{rms}} and IrmsI_{\text{rms}} are not provided, we would need this information to calculate the power.