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Alternating Current Test - 18

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Alternating Current Test - 18
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  • Question 1
    1 / -0
    An inductor $$20$$ mH, a capacitor $$100$$ $$\mu$$F and a resistor $$50$$ $$\Omega$$ are connected in series across a source of emf, V$$=10$$ $$\sin 314$$t. The power loss in the circuit is?
    Solution
    $$L = 20 mH$$ $$C = 100 \mu F$$ $$R = 50 \Omega$$
    $$V = 10 sin(314 t)$$
    $$V_0= 10$$, $$\omega = 314$$
    $$X_L = wL= 314 \times 20\times 10^{-3}= 6.28 \Omega$$
    $$X_C = \dfrac{1}{\omega C}=31.8 \Omega$$
    $$Z = \sqrt{R^2 + (X_C- X_L)^2} = 56.1 $$
    $$Power \ loss P=\dfrac{V_0^2 R}{2 Z^2}= 0.79 W$$


  • Question 2
    1 / -0
    A coil has resistance $$30   ohm$$ and inductive reactance $$20   ohm$$ at $$50   Hz$$ frequency. If an $$ac$$ source of $$200   volt,  100   Hz$$, is connected across the coil, the current in the coil will be
    Solution
    If $$\omega = 50 \times 2\pi$$  then  $$\omega L = 20\Omega$$
    If $${\omega}^{\prime} = 100 \times 2\pi$$  then  $${\omega}^{\prime} L = 40\Omega$$
    $$I = \displaystyle\frac{200}{Z} \displaystyle\frac{200}{\sqrt{{R}^{2} + {\left({\omega}^{\prime}L\right)}^{2}}} = \displaystyle\frac{200}{\sqrt{{30}^{2} + {\left(40\right)}^{2}}}$$
    $$I = 4  A$$.
  • Question 3
    1 / -0
    A coil of self-inductance L is connected in series with a bulb B and an AC source. Brightness of the bulb decreases when
    Solution
    As the iron rod is inserted, the magnetic field inside the coil magnetizes the iron increasing the magnetic field inside it. Hence. the inductance of the coil increases. Consequently, the inductive reactance of the coil increases. As a result, a larger fraction of the applied AC voltage appears across the lnductor, leaving less voltage across the bulb. Therefore' the brightness of the light bulb decreases.
  • Question 4
    1 / -0
    A series R-C circuit is connected to an alternating voltage source. Consider two situation:
    (a) When capacitor is filled
    (b) When capacitor is mica filled
    Current through resister is i and voltage across capacitor is V then :
    Solution
    For series C-R circuit, the impedance $$Z=\sqrt{R^2+X_C^2}$$   where $$X_C=\frac{j}{\omega C}$$ and current $$I=V/Z$$
    When the capacitor is filled by mica, the capacitance will be increased. If C increases, $$X_C$$ decreases,  so the current will increase and 
    hence voltage across resistance increases and voltage across capacitor decreases. thus, $$V_a>V_b$$
  • Question 5
    1 / -0
    A $$40 \mu F$$ capacitor is connected to a $$200 V,\ 50 Hz \ ac$$ supply. The rms value of the current
    in the circuit is, nearly :
    Solution
    RMS value of applied voltage = $$200\  V$$

    Impedance of a capacitor is given by:
    $$X_c=\dfrac{1}{2\pi f C}$$

    Hence, rms current through it is:
    $$I_{rms}=\dfrac{V}{X_C}$$

    $$I_{rms}=200 \times 2 \times \pi \times 50 \times 40 \times 10^{-6}$$

    $$I_{rms}=2.51 \ A$$
  • Question 6
    1 / -0
    A condenser of $$250\mu F$$ is connected in parallel to a cell of inductance $$0.16$$ mH, while its effective resistance is while its. Determine the resonant frequency.
    Solution
    Given 
    Capacitance, $$C= 250\mu F= 250\times 10^{-6} F$$
    Inductance , $$L=0.16mH= 0.16 \times 10^{-3}H$$

    Resonant frequency ,  $$f=\dfrac1{2\pi \sqrt{LC}}= \dfrac1{2\times 3.14\times \sqrt{250\times  10^{-6} \times 0.16 \times 10^{-3}}}= 8\times 10^5 Hz$$
  • Question 7
    1 / -0
    In a series LCR circuit, the voltage across the resistance, capacitance and inductance is $$10\ V$$ each. If the capacitance is short circuited the voltage across the inductance will be :
    Solution
    Since the voltages are all equal, the impedance of all the elements is same.

    $$R=X_L=X_C$$

    Total voltage in the circuit=$$I\sqrt{R^2+(X_L-X_C)^2}=IR=10V$$

    When capacitance is shorted, 

    $$I=\dfrac{V}{\sqrt{R^2+X_L^2}}=\dfrac{10}{\sqrt{2}R}$$

    Potential drop across inductor=$$IX_L=IR=\dfrac{10}{\sqrt{2}}V$$
  • Question 8
    1 / -0
    Reciprocal of Impedance is:
    Solution
    Impedance is the opposition a circuit presents to a current when a voltage is applied.
    Admittance is a measure of how easily a circuit or device will allow a current to flow.
    Admittance is defined as $$Y=\dfrac{1}{Z}$$
    where $$Z$$ is the impedance of the circuit.
  • Question 9
    1 / -0
    A $$10\ \mu F$$ capacitor is connected across a $$200\  V$$, $$ 50 \ Hz$$ A.C. supply. The peak current through the circuit is :
    Solution
    RMS value of applied voltage = $$200\  V$$

    Impedance of a capacitor is given by:
    $$X_C=\dfrac{1}{2\pi f C}$$

    Hence, rms current through it is:
    $$I=\dfrac{V}{X_C}$$
    $$I=200 \times 2 \times \pi \times 50 \times 10 \times 10^{-6}$$
    $$I=0.2 \pi \ A$$

    Peak current, $$I_{max}=\sqrt 2 I$$
    $$=0.628 \sqrt 2\ A$$
  • Question 10
    1 / -0
    The instantaneous value of emf and current in an A.C. circuit are $$E=1.414$$sin( $$100\pi t-\frac{\pi }{4} $$) , $$ I=0.707$$ sin($$100\pi t$$) . The resistance of the circuit is
    Solution
    resistance = impedance$$\times cos(\frac{\pi}{4})$$
    $$= \frac{1.414}{0.707}\times \frac{1}{\sqrt{2}}$$
    $$= \sqrt{2} \Omega$$
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