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Alternating Current Test - 47

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Alternating Current Test - 47
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  • Question 1
    1 / -0
    An inductor (L = 20 H), a resistor (R = 100 $$\Omega$$) and a battery (E = 10 V) are connected in series. After a long time, the circuit is short-circuited and then the battery is disconnected. Find the current in the circuit at 1 ms after short circuiting.
    Solution
    Given data :
    $$L = 20 H $$
    $$R = 100 \Omega$$
    $$E = 10 V$$
    Time after short circuiting the circuit, $$t = 1 ms.$$
    The initial current, $$I'$$ in the circuit is,
    $$I' = \dfrac{E}{R}$$

    $$I' = \dfrac{10}{100}$$

    $$I' = 0.1 A$$                 ........(1)

    The time constant, $$\tau$$ is,
    $$\tau = \dfrac{L}{R}$$

    $$\tau = \dfrac{20}{100}$$

    $$\tau = 0.2 s$$           ........(2)

    Now, the current at $$t = 1\ ms = 0.001\ s$$, is:
    $$I = I' e^{-\dfrac{t}{\tau}}$$

    Using equations (1) and (2) here, we get:
    $$I = (0.1)(e^{-\dfrac{0.001}{0.2}})$$
    $$I = (0.1)(e^{-0.005})$$
    $$I = (0.1)(0.995)$$
    $$I = 0.0995 A$$
    $$I = 9.95 \times 10^{-2} A$$
  • Question 2
    1 / -0
    In a series RLC circuit that is operating above the resonant frequency, the current
    Solution
    Capacitive reactance is given by  $$X_C = \dfrac{1}{wC}$$
    Inductive reactance is given by  $$X_L = wL$$
    At resonance,   $$X_L = X_C$$     $$\implies \ wL = \dfrac{1}{wC}$$
    But a frequency higher than resonance frequency,  $$X_L > X_C$$
    So the circuit behaves as a inductive circuit at a frequency higher that resonant frequency and the current lags behind the voltage in an inductive circuit.
    Thus option A is correct.
  • Question 3
    1 / -0
    If a capacitance C is connected in series with an inductor of inductance L, then the angular frequency will be
    Solution
    The peak current of an $$RLC$$ circuit is $$\frac{1}{\sqrt{R^{2}+(\frac{1}{{\omega C}}-\omega L)^{2}}}$$ , where $$\omega$$ is angular frequency
    It varies maximum when 
    We can get the angular frequency by equating $$\frac{1}{\omega C}-\omega L=0$$
    $$\Rightarrow \dfrac{1}{\omega C}=\omega L$$
    $$\Rightarrow \omega^2=\dfrac{1}{LC}$$
    $$\omega=\dfrac{1}{\sqrt{LC}}.$$
  • Question 4
    1 / -0
    A resistor of $$3 k \Omega$$, a $$0.05 \mu F$$ capacitor and a $$120 mH$$ coil are in series across a $$5 kHz, 20 V$$ ac source.What is the impedance, expressed in polar form?
    Solution

    Given,

    Resistance, $$R = 3 \, k\Omega = 3000 \Omega$$

    Capacitance, $$C = 0.05 \, \mu F = 0.05 \times 10^{-6} \, F$$

    Inductance, $$L = 120 \, mH = 120 \times 10^{-3} \, H$$

    $$f = 5 \, kHz = 5000 \, Hz$$

    It is asked to find the impedance in polar form

    We have ,

    Impedence, $$Z = \sqrt{R^2 + (X_L – X_C)^2}$$

    Also

    Inductive Reactance, $$X_L = L \omega  , X_C = \dfrac{1}{C \omega}$$

    We have $$\omega = 2 \pi F = 2 \times 3.14 \times 5000 = 31416$$

    $$X_L = L \omega = 120 \times 10^{-3} \times 31416 = 3769.9 $$

    Capacitive Reactance, $$X_C = \dfrac{1}{C \omega} = \dfrac{1}{31416 \times 0.05 \times 10^{-6}} = 636.61 $$

    $$Z = \sqrt{3000^2 + (3769.9 – 636.61)^2} = \sqrt{9000,000 + 9819090.9} = 4337.2 \approx 4337  \Omega $$


  • Question 5
    1 / -0
    A $$12 \Omega$$  resistor, a $$40 \mu F$$ capacitor, and an $$8 mH$$ coil are in series across an ac source. The resonant frequency is
    Solution
    $$\omega=\dfrac{1}{\sqrt{LC}}=\dfrac{1}{\sqrt{8\times 10^{-3}\times 40\times 10^{-6}}}$$

    $$\implies \omega=\dfrac{10^4}{\sqrt{32}}$$

    $$\omega=2\pi\nu$$      where $$\nu$$=frequency

    frequency$$=\nu=\dfrac{\omega}{2\pi}=\dfrac{10^4}{2\times 3.143\times \sqrt{32}}$$

    $$\implies \nu=281Hz$$

    Answer-(B)
  • Question 6
    1 / -0
    Which one of the following graphs in following figure represents variation of reactance $$'X_c'$$ of a capacitor with frequency 'f' of an ac supply?
    Solution
    Capacitor reactance is given by: $$X_c = \dfrac{1}{2\pi f C}, C$$ is the capacitance. 
    $$X_c\  \&\  f$$ are inversely proportional. 
  • Question 7
    1 / -0
    If the value of C in a series RLC circuit is decreased, the resonant frequency
    Solution
    Resonant frequency in the series RLC circuit    $$\nu_r = \dfrac{1}{2\pi\sqrt{LC}}$$
    $$\implies \ \nu_r\propto \dfrac{1}{\sqrt{C}}$$
    Thus resonant frequency of the circuit increases if the value of $$C$$ decreases.
  • Question 8
    1 / -0
    For a certain load, the true power is $$150 W$$ and the reactive power is $$125 W$$. The apparent power is
    Solution
    True power $$P  = 150 W$$
    Reactive power $$P_r = 125 W$$
    Thus apparent power $$P_a = \sqrt{P^2 + P_r^2}$$
    $$\therefore$$ $$P_a = \sqrt{(150)^2+ (125)^2}$$
    $$\implies$$ $$P_a = 195.2 W$$
  • Question 9
    1 / -0
    A $$90 \Omega$$ resistor, a coil with $$30 \Omega$$ of reactance, and a capacitor with $$50 \Omega$$  of reactance are in series across a $$12 V$$ ac source. The current through the resistor is
    Solution
    Resistance=$$R=90\Omega$$

    Reactance of coil$$=X_L=30\Omega$$

    Reactance of capacitor$$=X_C=50\Omega$$

    Impedance of circuit$$=X=\sqrt{R^2+(X_C-X_L)^2}$$

    $$\implies X=\sqrt{90^2+(50-30)^2}=\sqrt{8100+400}$$

    Current$$=I=\dfrac{E}{X}=\dfrac{12}{\sqrt{8500}}$$

    $$\implies I=0.13A=130mA$$

    Answer-(D)
  • Question 10
    1 / -0
    In a series RC circuit, when the frequency and the resistance are halved, the impedance
    Solution
    Capacitive reactance is given by  $$X_C = \dfrac{1}{2\pi f  C}$$
    where $$f$$ is the frequency.
    Impedance of the RC circuit   $$Z = \sqrt{R^2 + X_C^2} = \sqrt{R^2 + \dfrac{1}{4\pi^2 f^2 C^2}}$$
    If frequency and resistance are halved, we cannot determined unless the values are given.
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