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Alternating Current Test - 51

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Alternating Current Test - 51
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  • Question 1
    1 / -0
    A 44mH inductor is connected to a 220V, 50Hz AC supply. Then, the inductive reactance of the inductor is :
    Solution
    Inductive reactance $$X_L$$ is given by
    $$X_L = \omega L = 2\pi fL$$
    Given, f=50Hz, L=44mH 
    $$= 44\times 10^{-3}H$$
    $$X_L = 2\pi \times 44 \times 10^{-3} \times 50= 13.82 \Omega$$
  • Question 2
    1 / -0
    In the given circuit $$R$$ in pure resistance and $$X$$ is unknown circuit element. An AC voltage source is applied across $$A$$ and $$C$$. If $${ V }_{ AB }={ V }_{ AC }$$, then $$X$$ is

    Solution
    Since the voltage across the resistive element is same as the voltage applied, the voltage drop across $$BC$$ is zero. This is possible only when the ohmic value of the element connected across $$BC$$ is zero. So, $$X$$ should be combination of inductance and capacitance at resonance.
  • Question 3
    1 / -0
    The frequency of the output signal becomes ________ times by doubling the value of the capacitance in the LC oscillator circuit.
    Solution
    In the L-C circuits
    For the first condition
    $${ f }_{ 1 }=\dfrac { 1 }{ 2\pi  } \sqrt { \dfrac { 1 }{ LC }  } $$            .....(i)
    For the second condition, when $$C=$$ doubling
    $${ f }_{ 2 }=\dfrac { 1 }{ 2\pi  } \sqrt { \dfrac { 1 }{ 2LC }  } $$                ....(ii)
    From the equation (i), we get
    $${ f }_{ 2 }=\dfrac { 1 }{ 2\pi  } \sqrt { \dfrac { 1 }{ LC }  } \times \dfrac { 1 }{ \sqrt { 2 }  } \Rightarrow { f }_{ 2 }={ f }_{ 1 }\times \dfrac { 1 }{ \sqrt { 2 }  } $$
    So, the frequency of the output signal becomes $${ 1 }/{ \sqrt { 2 }  }$$ times by doubling the value of the capacitance in the L-C oscillator circuit.

  • Question 4
    1 / -0
    In a series resonant circuit, the AC voltage across resistance R, inductor L and capacitor C are 5 V, 10 V and 10 V respectively. The AC voltage applied to the circuit will be 
    Solution
    Given, $$V_R=5\, V, V_L=10$$ and $$V_C=10 \, V$$
    In the MR circuit, the AC voltage applied to the circuit will be 
    $$V=\sqrt{V^2_R+(V_L-V_C)^2}$$
    $$=\sqrt{(5)^2+(10-10)^2}$$
    $$=5\, V$$

  • Question 5
    1 / -0
    The diagram given show the variation of voltage and current in an AC circuit. The circuit contains

    Solution
    The given circuit shows that the current lags the applied voltage. This is possible if the circuit has inductive element. So, the circuit contain a pure inductor.
  • Question 6
    1 / -0
    The power loss in an AC circuit can be minimized by.
    Solution
    In an AC circuit, power loss can be minimized by decreasing in resistance and by increasing in inductance.
  • Question 7
    1 / -0
    What is the range of the characteristic impedance of a coaxial cable?
    Solution
    Characteristic impedance of a coaxial cable is between $$50\Omega$$ to $$70\Omega$$.
  • Question 8
    1 / -0
    A $$220$$V main supply is connected to a resistance of $$100$$k$$\Omega$$. The effective current is?
    Solution
    Effective current is the rms value. Here, $$220$$V is the labelled value of AC which is also the rms value. Hence,
    $$I_{rms}=\displaystyle\frac{E_{rms}}{R}$$
    $$I_{rms}=\displaystyle\frac{220}{100\times 10^3}$$
    $$I_{rms}=2.2mA$$.
  • Question 9
    1 / -0
    Which one of the following curves represents variation of current i with frequency f in series LCR circuit?
    Solution
    In series LCR circuit, the graph(c) represents the curve between current (i) and frequency(f).
  • Question 10
    1 / -0
    Consider two series resonant circuits with components $$L_1C_1$$ and $$L_2C_2$$ with same resonant frequency , $$\omega$$.When connected in series, the resonant frequency of the combination is 
    Solution
    Initially, $$\omega = \dfrac{1}{\sqrt{L_1C_1}}$$ and 

                 $$\omega = \dfrac{1}{\sqrt{L_2C_2}}$$

    Finally, $$L_{eq} = L_1 + L_2$$

                 $$C_{eq} = \dfrac{C_1C_2}{C_1 + C_2}$$          

    $$\omega' = \dfrac{1}{\sqrt{L_{eq}C_{eq}}}$$

    from above equation, we will get $$\omega' = \omega$$
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