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Alternating Current Test - 32

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Alternating Current Test - 32
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  • Question 1
    1 / -0
    In the series L-C-R circuit figure, the voltmeter and ammeter readings are

    Solution
    Here, $$V_L=V_C$$.

    $$V_L$$ and $$V_C$$ are in oppositr phases. Hence they will cancel each other. Now the resultant potential difference is equal to the applied potential difference. 

    i.e. $$V=100V$$ 

    Impedence, $$Z=R(X_L \, or \, X_C)$$

    Therefore,

    $$I_{rms}=\dfrac{V_{rms}}{Z}=\dfrac{V_{rms}}{R}=\dfrac{100}{50}=2\,A$$

    So, the voltmeter reading is $$100\,V$$ and ammeter reading is $$2\,A$$.

  • Question 2
    1 / -0
    A resistor $$R$$ and capacitor $$ C$$ are connected in series across an AC source of rms voltage $$5 V$$. If the rms voltage across $$C$$ is $$3 V$$ then that across $$R$$ is :
    Solution
    Source voltage = $$\sqrt{(Capacitor\ voltage)^2+(Resistor \ voltage)^2}$$

    $$[V_{s(rms)}]^2 = [V_{C(rms)}]^2+[V_{R(rms)}]^2$$

    $$(5)^2 = (3)^2+[V_{R(rms)}]^2$$

    $$25-9 = [V_{R(rms)}]^2$$

    $$16 = [V_{R(rms)}]^2$$

    $$ V_{R(rms)}=4V$$
  • Question 3
    1 / -0
    The potential difference between the ends of a resistance R is $$V_{R}$$, between the ends of capacitor is $$V_{C}$$ $$=$$ 2$$V_{R}$$ and between the ends of inductance is $$V_{L}$$ $$=$$ 3$$V_{R}$$ then the alternating potential of the source in terms of $$V_{R}$$ will be:
    Solution
    $$V_S = \sqrt{V_R^2+(V_L-V_C)^2}$$

    $$= \sqrt{V_R^2+(3V_R-2V_R)^2}$$

    $$= \sqrt{V_R^2+V_R^2}$$

    $$= V_R \sqrt{2}$$.
  • Question 4
    1 / -0
    The natural frequency of an LC - circuit is $$1,25,000$$ cycles per second. Then the capacitor C is replaced by another capacitor with a dielectric medium of dielectric constant k. In this case, the frequency decreases by $$25 kHz$$. The value of k is:
    Solution

    Natural frequency $$= 125000 Hz$$

    New frequency $$= 125000 - 25000$$

                           $$ = 100000 Hz$$

    Frequency of L-C circuit

    $$2\pi f = \dfrac{1}{\sqrt{LC}}$$

    So, $$2\pi f_1 = \dfrac{1}{\sqrt{LC_1}}$$   ---(1)

    $$2\pi f_2 = \dfrac{1}{\sqrt{LC_2}}$$   ---(2)

    Dividing (1) by (2)

    $$\dfrac{f_1}{f_2} = \sqrt{\dfrac{C_2}{C_1}}$$

    $$\sqrt{\dfrac{C_2}{C_1}} = \dfrac{125000}{100000} = \dfrac{5}{4}$$

    $$\dfrac{C_2}{C_1} = \dfrac{25}{16}$$

    $$k = \dfrac{C_2}{C_1} = \dfrac{25}{16} = 1.56$$

  • Question 5
    1 / -0
    In the following circuit, the values of current flowing in the circuit at f=0 and f=$$\infty$$ will respectively be

    Solution
    In a LCR circuit current at $$t = 0$$ is zero because inductor does not allow flow of current,
    and at $$t = \infty$$ also current is zero because capacitor does not allow flow of current.
  • Question 6
    1 / -0
    The reading of voltmeter and ammeter in the following figure will respectively be :

    Solution

    In the problem $$X_C = 4\Omega$$
    and $$X_L = 4\Omega$$
    So, V across $$X_C$$ and $$X_L$$ will be same and in opposite direction, So net voltage will be zero. Since voltmeter is connected parallel to Capacitor and inductor so, it will read 0 volts.

    Current $$=$$ $$\dfrac{V}{impedance}$$

    $$impedence= \sqrt { R^{2}+X_L^{2} }  $$

    Current$$= \dfrac{90} {\sqrt{45^{2}+4^{2}}}$$

    $$= \dfrac{90}{45.17}$$   $$\simeq 2$$A.

  • Question 7
    1 / -0
    In the following diagram, the value of emf of A.C. source will be :

    Solution
    $$ E_{rms} = \sqrt{ V_R^2 + ( V_L - V_c )^2 } $$

    $$= \sqrt{ 40^2 + (40-80)^2}$$

    $$ = \sqrt{ 40^2 + 40^2} $$

    $$= 40 \sqrt{2}  V $$
  • Question 8
    1 / -0
    An inductance of 0.2 H and a resistance of 100$$\Omega $$ are connected in series to an A.C. 180 V, 50 Hz supply. The apparent current flowing in the circuit will be
    Solution
    $$Z= \sqrt{X_L^2+R^2}$$

    $$= \sqrt{(2\pi fL)^2+R^2}$$

    $$= \sqrt{(2\pi 50\times 0.2)^2+(100)^2}$$

    $$= \sqrt{13947.84}$$

    $$= 118.1 \Omega$$

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

    $$= \dfrac{180}{118.1}$$

    $$= 1.525A$$
  • Question 9
    1 / -0
    An $$LCR$$ circuit has $$L=10\ mH, R=3\Omega$$, and $$C =1\mu$$ $$F$$ connected in series to a source of $$15 \cos\omega t$$ volt. The current amplitude at a frequency that is $$10\%$$ lower than the resonant frequency is:
    Solution
    Resonant frequency, $$w_o=\dfrac{1}{\sqrt{LC}}=\dfrac{1}{\sqrt{(10\times 10^{-3})(10^{-6})}}=10^4 rad/s$$

    New frequency, $$\omega=(0.9)\omega_o=9\times 10^3 rad/s$$

    We have new $${ X }_{ L }=\omega L=9\times { 10 }^{ 3 }\times 10\times { 10 }^{ -3 }=90\Omega $$ and $$X_C= \dfrac {1}{\omega C}=111.11$$ $$ohm$$.

    Thus we calculate new $$Z$$ as

    $$\sqrt{3^2+[90-111.11]^2}$$

    $$=21.32 \Omega$$

    Current amplitude $$=\dfrac{V_o}{Z}=\dfrac{15}{21.32}=0.7  A$$
  • Question 10
    1 / -0
    The values of $$X_{L}, X_{C}$$ and R in series with an A.C.  circuit are 8$$\Omega $$ , 6$$\Omega $$ and 10$$\Omega $$ respectively. The
    total impedance of the circuit will be ________$$\Omega $$
    Solution
    $$Z = \sqrt{R^2+(X_L-X_C)^2}$$

    $$= \sqrt{(10)^2+(8-6)^2}$$

    $$= \sqrt{10^2+2^2}$$

    $$= \sqrt{100+4}$$

    $$= 10.2 \Omega$$
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