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Alternating Current Test - 21

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Alternating Current Test - 21
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  • Question 1
    1 / -0
    The phase difference between alternating emf and current in a purely capacitive circuit will be
    Solution
    In a purely capacitive circuit, current leads the voltage by $$\pi /2 $$.
  • Question 2
    1 / -0

    The square root of the product of inductance and capacitance has dimensions of

    Solution
    $$\displaystyle f = \dfrac{1}{\sqrt{LC}}   $$

    $$ or  \ \ \  \sqrt{LC} = T$$
  • Question 3
    1 / -0
    The resonant frequency in an anti resonant circuit is :
    Solution
    For resonance

    $${ X }_{ L }={ X }_{ C }$$

    $$\omega L=\dfrac { 1 }{ \omega C } $$

    $${ \omega  }^{ 2 }=\dfrac { 1 }{ LC } $$

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

    $$2\pi f=\dfrac { 1 }{ \sqrt { LC }  } $$

    $$f=\dfrac { 1 }{ 2\pi \sqrt { LC }  } $$
  • Question 4
    1 / -0
    In an A.C. circuit, the potential difference across an inductance and a resistance joined in series are respectively $$16 V$$ and $$20 V$$. The total potential difference across the circuit is
    Solution
    Total potential = $$\sqrt{V_R^2+V_L^2}$$

    $$= \sqrt{(16)^2+(20)^2}$$

    $$= \sqrt{256+400}$$

    $$= \sqrt{656}$$

    $$= 25.6V$$
  • Question 5
    1 / -0
    An LCR series circuit contains $$L = 8 H$$, C$$=$$0.5 $$\mu $$ F and R $$=$$ 100$$\Omega $$ .The resonant frequency of the circuit is
    Solution
     For resonant frequency reactance should be zero.
    So, $$X_L-X_C = 0$$
    $$X_L = X_C$$
    $$\omega L = \dfrac{1}{\omega C}$$
    $$\implies \ \omega  = \sqrt{\dfrac{1}{2C}}$$
    Or  $$2\pi f = \dfrac{1}{\sqrt{2C}}$$
    Thus resonant frequency  $$f = \dfrac{1}{2\pi}\times \dfrac{1}{\sqrt{2C}}$$
    $$f= \dfrac{1}{2\pi}\times \dfrac{1}{\sqrt{8\times 0.5\times 10^{-6}}}$$
    $$f= \dfrac{1}{2\pi}\times \dfrac{10^3}{2}$$
    $$f= \dfrac{250}{\pi}Hz$$
  • Question 6
    1 / -0
    In the circuit shown, a 30 V d.c source gives a current 2.0A as recorded in the ammeter A and 30V a.c. source of frequency 100Hz gives a current 1.2A. The inductive reactance is 

    Solution
    In DC current

    $$V = iR$$

    $$\dfrac{V}{i} = R$$

    $$R = \dfrac{30}{2} = 15\Omega$$

    In a.c. current

    $$V = i Impedance$$

    $$\dfrac{V}{i} = Impedance$$

    $$Impedance = \dfrac{30}{1.2} = 25\omega$$

    $$Impedance = \sqrt{R^2+(X_L)^2}$$

    $$(25)^2 = R^2+(X_L)^2$$

    $$X_L = \sqrt{(25)^2-R^2}$$

    $$= \sqrt{625-225}$$

    $$= \sqrt{400}$$

    $$= 20\Omega$$
  • Question 7
    1 / -0
    If the values of inductance and frequency in an AC circuit are 2 henry and $$\displaystyle \dfrac{10^3}{2\pi}$$ Hz respectively then the value of inductive reactance will be
    Solution
    Inductive reactance $$= L\omega =2\times 2\pi \dfrac { { 10 }^{ 3 } }{ 2\pi  } =2\times { 10 }^{ 3 }\Omega $$
  • Question 8
    1 / -0
    .In the given circuit, the phase difference between voltages across R and C is 

    Solution
    Voltage phase difference between R and C is $$\dfrac{\pi}{2}$$  ,
    R and L is $$\dfrac{\pi}{2}$$ and, L and C is $$\pi$$ for a LCR circuit such that voltage in L leads by $$\dfrac{\pi}{2}$$ from voltage in R and voltage in R leads by $$\dfrac{\pi}{2}$$ from voltage in C.
  • Question 9
    1 / -0
    An experimentalist has a coil of 3 mH. He wants to make a circuit whose frequency is 106 Hz. The capacity of condenser used will be
    Solution
    Circuit has to work properly at resonance therfore,

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

    $$C=\dfrac { 1 }{ { \omega  }^{ 2 }L } $$

    $$C=\dfrac { 1 }{ 4\pi ^{ 2 }f^2L } $$

    $$C=\dfrac { 1 }{ 4\pi ^{ 2 }\times 106^2\times 3\times { 10 }^{ -3 } } $$

    $$C=752.22\mu F$$
  • Question 10
    1 / -0
    The phase difference between the applied emf and the line current in an anti resonant circuit at resonance is
    Solution
    We know that phase difference is given by:

    $$\phi =\arctan { (\dfrac { ({ X }_{ L }-{ X }_{ c }) }{ R } ) } $$

    at resonance

    $${ X }_{ L }-{ X }_{ c }=0$$

    Therefore  $$\phi =0$$.
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