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Alternating Current Test - 34

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Alternating Current Test - 34
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  • Question 1
    1 / -0
    For a series LCR circuit the power loss at resonance is : -
    Solution

  • Question 2
    1 / -0
    The natural frequency of the circuit shown in fig. is

    Solution
    Leq=L+L=2L L_{eq}=L+L=2L

      Ceq=C/2     C_{eq}=C/2

    naturalfrequency=1LeqCeq \therefore natural frequency = \dfrac{1}{\sqrt {L_{eq} C_{eq} }}
  • Question 3
    1 / -0
    The capacitance in an oscillatory LC circuit is increased by 1%. The change in inductance required to restore its frequency of oscillation is to
    Solution
     ωr=constant \omega_r=constant

    LC=constant \Rightarrow LC=constant

    LdC+CdL=0\Rightarrow LdC+CdL=0

    dLL=dCC=1\Rightarrow \dfrac {dL}{L}=-\dfrac {dC}{C}=-1 % 
  • Question 4
    1 / -0
    In alternating current
    Solution

    C

    Electric charge in alternating current (AC) changes direction periodically. The voltage in AC circuits also periodically reverses because the current changes direction.

     

  • Question 5
    1 / -0
    The frequency of A.C mains in India is
    Solution
    In India, the AC mains supply is referred to as single-phase alternating current and corresponds to a voltage of 230 V at a frequency of 50Hz50 Hz, similar to most European countries. Whereas in the USA, AC mains supply uses 60Hz60 Hz
  • Question 6
    1 / -0
    An inductor, a resistor and a capacitor are joined in series with an AC source. As the frequency of the source is slightly increased from a very low value, the reactance
    Solution

    A

    Resonance of inductor, XL=2πfLX_L = 2 \pi f L

    Here f is the frequency of Ac, L is inductance of inductor. Reactance is directly proportional to frequency. Therefore, with increase in frequency reactance also increases.

    When current passes through inductor, magnetic field develop across inductor, magnetic field cut by inductor and emf is induced. This emf is called back emf which opposes the applied emf. Back emf increase with increase in frequency of applied emf. Therefore opposition, i.e. reactance also increases with increase in frequency. 

  • Question 7
    1 / -0
    The circuit shown in Fig. acts as a 

    Solution
    The circuit shown in figure has capacitor and inductor in parallel so their will be current flowing continuously with energy being transformed into electrical in capacitor and magnetic in inductor, hence it is a tuned filter.
  • Question 8
    1 / -0
    A steady potential difference of 100 V produces heat at a constant rate in a resistor. The alternating voltage which will produce half the heating effect in the same resister will be
    Solution
    The power supplied to the resistor by DC source =Vdc2R=\dfrac{V_{dc}^2}{R}
    Energy given by AC source =0TV02Rdt=\int_0^T \dfrac{V_0^2}{R}dt 

    Hence, 0TV02sin2ωtRdt=12×Vdc2TR\int_0^T \dfrac{V_0^2sin^2\omega t}{R}dt=\dfrac{1}{2}\times \dfrac{V_{dc}^2T}{R} 

        V0=Vdc=100V\implies V_0=V_{dc}=100V
  • Question 9
    1 / -0

    An amplitude modulated (AM) radio operates at 550kHz550 kHz to 1650kHz1650 kHz. If LL is fixed and CC is varied for tuning then minimum and maximum value of CC is

    Solution
    fmaxfmin=3\displaystyle \frac{f_{max}}{f_{min}} = 3

    LCmaxLCmin=3 \therefore \dfrac{\sqrt{LC_{max}}}{\sqrt{LC_{min}}} = 3

    CmaxCmin=9\dfrac{C_{max}}{C_{min}}= 9

    Cmin=CC_{min}= C

    Cmax=9C\therefore C_{max}=9C
  • Question 10
    1 / -0
    When 4 V4\ V DC is connected across an inductor, current is 0.2 A0.2\ A. When AC of 4 V4\ V is applied the current is 0.1 A0.1\ A. Then self inductance of the coil is:
    [Given ω=1000  rads1\omega = 1000\  rads^{-1}]
    Solution
    Z=40.1=40 Ω=R2+(Lω)2\displaystyle Z = \frac{4}{0.1} = 40\ \Omega = \sqrt{R^2 + (L\omega)^2}

    and R=40.2=20 Ω\displaystyle R = \frac{4}{0.2} = 20\ \Omega

     Lω=203Ω\displaystyle \therefore\ L\omega = 20\sqrt3 \Omega

    or L=203 mH\displaystyle L = 20\sqrt3\ mH
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