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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 2020 mH, a capacitor 100100 μ\muF and a resistor 5050 Ω\Omega are connected in series across a source of emf, V=10=10 sin314\sin 314t. The power loss in the circuit is?
    Solution
    L=20mHL = 20 mH C=100μFC = 100 \mu F R=50ΩR = 50 \Omega
    V=10sin(314t)V = 10 sin(314 t)
    V0=10V_0= 10, ω=314\omega = 314
    XL=wL=314×20×103=6.28ΩX_L = wL= 314 \times 20\times 10^{-3}= 6.28 \Omega
    XC=1ωC=31.8ΩX_C = \dfrac{1}{\omega C}=31.8 \Omega
    Z=R2+(XCXL)2=56.1Z = \sqrt{R^2 + (X_C- X_L)^2} = 56.1
    Power lossP=V02R2Z2=0.79WPower \ loss P=\dfrac{V_0^2 R}{2 Z^2}= 0.79 W


  • Question 2
    1 / -0
    A coil has resistance 30 ohm30   ohm and inductive reactance 20 ohm20   ohm at 50 Hz50   Hz frequency. If an acac source of 200 volt, 100 Hz200   volt,  100   Hz, is connected across the coil, the current in the coil will be
    Solution
    If ω=50×2π\omega = 50 \times 2\pi  then  ωL=20Ω\omega L = 20\Omega
    If ω=100×2π{\omega}^{\prime} = 100 \times 2\pi  then  ωL=40Ω{\omega}^{\prime} L = 40\Omega
    I=200Z200R2+(ωL)2=200302+(40)2I = \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 AI = 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=R2+XC2Z=\sqrt{R^2+X_C^2}   where XC=jωCX_C=\frac{j}{\omega C} and current I=V/ZI=V/Z
    When the capacitor is filled by mica, the capacitance will be increased. If C increases, XCX_C decreases,  so the current will increase and 
    hence voltage across resistance increases and voltage across capacitor decreases. thus, Va>VbV_a>V_b
  • Question 5
    1 / -0
    A 40μF40 \mu F capacitor is connected to a 200V, 50Hz ac200 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:
    Xc=12πfCX_c=\dfrac{1}{2\pi f C}

    Hence, rms current through it is:
    Irms=VXCI_{rms}=\dfrac{V}{X_C}

    Irms=200×2×π×50×40×106I_{rms}=200 \times 2 \times \pi \times 50 \times 40 \times 10^{-6}

    Irms=2.51 AI_{rms}=2.51 \ A
  • Question 6
    1 / -0
    A condenser of 250μF250\mu F is connected in parallel to a cell of inductance 0.160.16 mH, while its effective resistance is while its. Determine the resonant frequency.
    Solution
    Given 
    Capacitance, C=250μF=250×106FC= 250\mu F= 250\times 10^{-6} F
    Inductance , L=0.16mH=0.16×103HL=0.16mH= 0.16 \times 10^{-3}H

    Resonant frequency ,  f=12πLC=12×3.14×250× 106×0.16×103=8×105Hzf=\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 V10\ 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=XL=XCR=X_L=X_C

    Total voltage in the circuit=IR2+(XLXC)2=IR=10VI\sqrt{R^2+(X_L-X_C)^2}=IR=10V

    When capacitance is shorted, 

    I=VR2+XL2=102RI=\dfrac{V}{\sqrt{R^2+X_L^2}}=\dfrac{10}{\sqrt{2}R}

    Potential drop across inductor=IXL=IR=102VIX_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=1ZY=\dfrac{1}{Z}
    where ZZ is the impedance of the circuit.
  • Question 9
    1 / -0
    A 10 μF10\ \mu F capacitor is connected across a $$200\  V$$, 50 Hz 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:
    XC=12πfCX_C=\dfrac{1}{2\pi f C}

    Hence, rms current through it is:
    I=VXCI=\dfrac{V}{X_C}
    I=200×2×π×50×10×106I=200 \times 2 \times \pi \times 50 \times 10 \times 10^{-6}
    I=0.2π AI=0.2 \pi \ A

    Peak current, Imax=2II_{max}=\sqrt 2 I
    =0.6282 A=0.628 \sqrt 2\ A
  • Question 10
    1 / -0
    The instantaneous value of emf and current in an A.C. circuit are E=1.414E=1.414sin( 100πtπ4100\pi t-\frac{\pi }{4} ) , I=0.707 I=0.707 sin(100πt100\pi t) . The resistance of the circuit is
    Solution
    resistance = impedance×cos(π4)\times cos(\frac{\pi}{4})
    =1.4140.707×12= \frac{1.414}{0.707}\times \frac{1}{\sqrt{2}}
    =2Ω= \sqrt{2} \Omega
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