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Alternating Current Test - 44

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Alternating Current Test - 44
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  • Question 1
    1 / -0
    220 V, 50 Hz, AC source is connected to an inductance of 0.2 H and a resistance of 20 $$\Omega$$ in series. What is the current in the circuit?
    Solution
    The frequency of AC source $$=f=50Hz$$
    Thus the impedance of the inductor, $$X_L=\omega L=(2\pi f)L=20\pi\Omega$$
    Resistance of the resistor $$=20\Omega$$
    Thus, the net impedance of the circuit $$=\sqrt{X_L^2+R^2}=65.94\Omega$$
    Thus, the current in the circuit $$=\dfrac{V}{X}=\dfrac{220V}{65.94\Omega}=3.33A$$
  • Question 2
    1 / -0
    In L-C-R circuit power of 3 mH inductance and $$4\Omega$$ resistance, EMF $$E=4\,cos\,1000t$$ volt is applied. The amplitude of current is
    Solution
    Impedance of inductor=$$X_L=\omega H=1000\times 3mH=3\Omega$$
    Thus the impedance of the circuit=$$X=\sqrt{X_{L}^2+R^2}=5\Omega$$
    Thus amplitude of current $$I_{max}=\dfrac{E_{max}}{X}=\dfrac{4V}{5\Omega}=0.8A$$
  • Question 3
    1 / -0
    The impedance of a circuit, when a resistance $$R$$ and an inductor of inductance $$L$$ are connected in series in an AC circuit of frequency $$f$$, is
    Solution
    The impedance due to the inductor is $$2\pi fL$$ and voltage drop across inductor leads the voltage drop across resistor by $$90°$$. 
    So, the net impedance will be: $$Z=\sqrt { { R }^{ 2 }+{ (2\pi fL) }^{ 2 } } $$
  • Question 4
    1 / -0
    The current through a coil of self-inductance $$L=2mH$$ is given by $$i=t^2e^{-t}$$ at time t. How long it will take to make the emf zero?
    Solution
    The current is given by the relation $$i=t^2e^{-t}$$.
    Hence the emf would be equal to
    $$e=-L\dfrac{di}{dt}=-2\times10^{-3}\times(2te^{-t}-t^2e^{-t})$$
    If the emf is zero, $$e=0$$, hence
    $$2te^{-t}=t^2e^{-t}\Rightarrow\,t=2\,s$$
  • Question 5
    1 / -0
    In an LCR circuit inductance is changed from $$L$$ to $$\dfrac{L}{2}$$. To keep the same resonance frequency, $$C$$ should be changed to
    Solution
    Resonance frequency, $$(f)=\dfrac{1}{2\pi \sqrt{LC}}$$
    For $$f$$ to be constant the product $$LC$$ must be constant.
    So, if we half the value of inductance then the value of capacitance must be $$doubled$$.
    $$C$$ should be changed to $$2C$$.
  • Question 6
    1 / -0
    The resonant frequency of an L-C circuit is
    Solution
    Resonance frequency $$f$$ of an L-C circuit can be written as 

    Resonance frequency, $$f =\dfrac{1}{2 \pi \sqrt{LC}}$$ where $$L$$= inductance and $$C$$ is capacitance 
  • Question 7
    1 / -0
    Resonance frequency of a circuit is $$f$$. If the capacitance is made $$4$$ times the initial value, then the resonance frequency will become
    Solution
    As  we know,
    Resonance frequency of a circuit
    $$f=\dfrac { 1 }{ 2\pi \sqrt { LC }  } $$
    ie, $$f\propto \dfrac { 1 }{ \sqrt { C }  } $$
    $$\Rightarrow \dfrac { { f }^{ \prime  } }{ f } =\dfrac { \sqrt { C }  }{ \sqrt { 4C }  } =\dfrac { 1 }{ 2 } $$
    $$\Rightarrow { f }^{ \prime  }=\dfrac { f }{ 2 } $$
  • Question 8
    1 / -0

    An oscillating circuit contains an inductor of inductance $$ { 10 }^{ -6 }$$ H and two capacitor each of capacitance $$5\times { 10 }^{ -6 }$$ farad connected in parallel. Then the resonance frequency of the circuit is

    Solution
    $$\omega =\dfrac { 1 }{ \sqrt { LC }  } =\dfrac { 1 }{ \sqrt { { 10 }^{ -6 }\times 2\times 5\times { 10 }^{ -6 } }  } $$

    $$=\sqrt { { 10 }^{ 11 } } \approx 3\times { 10 }^{ 5 }\\$$

    $$ f=\dfrac { \omega  }{ 2\pi  } =\dfrac { 3\times { 10 }^{ 5 } }{ 2\pi  } $$

    $$=\dfrac { { 1.5\times 10 }^{ 5 } }{ \pi  } $$
  • Question 9
    1 / -0
    An alternating emf given by equation $$E = 300 sin [(100\pi )t]$$ $$volt$$ is applied to a resistance $$100\ ohms$$. The rms current through the circuit is (in $$amperes$$):
    Solution
    Alternating emf equation            $$E = 300$$ $$ sin(100\pi t)$$
    $$\therefore$$   Peak emf       $$E_o = 300$$ $$volts$$
    The rms emf       $$E_{rms}  = \dfrac{E_o}{\sqrt{2}}  = \dfrac{300}{\sqrt{2}}$$ $$volts$$
    Value of resistance        $$R = 100\ \Omega$$

    $$\therefore$$ Value of rms current          $$I_{rms}  = \dfrac{E_{rms}}{R}  = \dfrac{300}{\sqrt{2} \times 100}   =\dfrac{3}{\sqrt{2}}$$ $$A$$
  • Question 10
    1 / -0

    When $$100\ volt\ DC$$ is applied across a solenoid, a current of $$1.0\ amp$$ flows in it. When $$100\ volt\ AC$$ is applied across the same coil, the current drops to $$0.5\ amp.$$ If the frequency of the AC source is $$50\ Hz$$ the impedance and inductance of the solenoid are:

    Solution
    We know that
    $$i=\frac { V }{ R } ,\quad for\quad DC\Rightarrow R=\frac { 100 }{ 1 } =100\Omega \\ i=\frac { V }{ L\omega  } ,\quad when\quad AC\quad is\quad applied\Rightarrow L\omega =\frac { V }{ i } =\frac { 100 }{ 0.5 } =200\Omega \\ L=\frac { 200 }{ 2\pi \times 50 } =0.055H$$
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