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Alternating Current Test - 41

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Alternating Current Test - 41
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  • Question 1
    1 / -0
    The adjoining figure shows an $$AC$$ circuit with resistance $$R$$, inductance $$L$$ and source voltage $$V_s$$. Then

    Solution
    $$\displaystyle V_S=\sqrt{V^2_R+V^2_L}$$
    $$=\displaystyle \sqrt{(70)^2+(20)^2}=72.8V$$
    $$\displaystyle \tan \phi=\frac{X_L}{R}=\frac{V_L}{V_R}=\frac{20}{70}=\frac{2}{7}$$
  • Question 2
    1 / -0
    In series $$L-C-R$$ circuit voltage drop across resistance is $$8V$$, across inductor is $$6V$$ and across capacitor is $$12V$$. Then
    Solution
    $$\displaystyle V=\sqrt{V^2_R+(V_C-V_L)^2}=10V$$
    $$V_C > V_L$$, hence current leads the voltage.
    Power factor $$\displaystyle =\cos \phi=\frac{8}{10}=0.8$$
  • Question 3
    1 / -0
    An $$AC$$ voltage is applied across a series combination of $$L$$ and $$R$$. If the voltage drop across the resistor and inductor are $$20V$$ and $$15V$$ respectively, then applied peak voltage is :
    Solution
    $$\displaystyle V=\sqrt{V^2_R+V^2_L}$$
    $$\displaystyle =\sqrt{(20)^2+(15)^2}=25V$$
    But this is the rms value.
    $$\therefore$$ Peak value $$=\displaystyle \sqrt 2 V_{rms}=25\sqrt 2V$$
  • Question 4
    1 / -0
    In the circuit shown in figure, the $$AC$$ source gives a voltage $$V=20\cos (2000t)$$. Neglecting source resistance, the voltmeter and ammeter readings will be

    Solution
    Here, $$X_{L}=\omega L=2000\times 5\times 10^{-3}\Omega =10\Omega$$
    $$X_{C}=\dfrac{1}{\omega C}=\dfrac{1}{2000\times 50\times 10^{-6}}\Omega=10\Omega$$
    $$X_{L}=X_{C}$$. Hence this is a case of resonance.
    $$\implies i=\dfrac{V}{R}=\dfrac{(20/\sqrt{2})}{10}=1.4A$$
    Voltmeter reading=$$1.4\times 4 volt=5.6V$$
  • Question 5
    1 / -0
    When $$100\space V$$ dc is applied across a solenoid, a current of $$1.0\space A$$ flows in it. When $$100\space V$$ ac is applied across the same coil, the current drops to $$0.5\space A$$. If the frequency of the ac source is $$50\space Hz$$, the impedance and inductance of the solenoid are
    Solution
    impedance= $$\frac{V_{ac}}{I_{ac}}= \frac {100 V}{0.5 A} = 200 \Omega $$
    R=$$ \frac{V_{dc}}{I_{dc}}=\frac{100}{1}=100 \Omega $$
    $$L \omega $$ = $$ \sqrt{ {impedance}^{2} - R^2 } = \sqrt { 200^2-100^2 } =173.2 $$
    $$L=\frac{173.2}{\omega}=\frac{173.2}{2\pi 50} =0.55 H $$
  • Question 6
    1 / -0
    An inductive coil has resistance of $$100\Omega$$. When an ac signal of frequency $$1000\space Hz$$ is fed to the coil, the applied voltage leads the current by $$45^{\small\circ}$$. What is the inductance of the coil?
    Solution
    $$ tan(45) = 1 =  \frac{L \omega}{R} $$
    $$ L = R / \omega = R / ( 2 \pi 1000) = .016 H$$

  • Question 7
    1 / -0
    In a series $$LC$$ circuit, the applied voltage is $$V_0$$. If $$\omega$$ is very low, then the voltage drop across the inductor $$V_L$$ and capacitor $$V_C$$ are

    Solution
    $$X_L=\omega L$$
    If $$\omega$$ is very low, then $$X_L=0$$
    $$\therefore V_L=0$$
    or $$V=V_C=V_0$$
  • Question 8
    1 / -0
    An $$AC$$ voltage source $$V=V_0\sin \omega t$$ is connected across resistance $$R$$ and capacitance $$C$$ as shown in the figure. It is given that $$R=1/\omega C$$ and the peak current is $$I_0$$. If the angular frequency of the voltage source is changed to $$\omega/\sqrt 3$$ then the new peak current in the circuit is

    Solution
    $$\displaystyle R=\frac{1}{\omega C}=X_C$$
    $$\displaystyle \therefore Z=\sqrt{R^2+X^2_C}=\sqrt 2 R$$  (as $$X_C=R$$)
    $$\displaystyle I_0=\frac{V_0}{Z}=\frac{V_0}{\sqrt 2 R}$$
    When $$\omega$$ becomes $$\displaystyle \frac{1}{\sqrt 3}$$ times, $$X_C$$ will become $$\sqrt 3$$ times or $$\sqrt 3R$$.
    $$\displaystyle Z'=\sqrt{(R^2)+(\sqrt 3R)^2}=2R$$
    $$\displaystyle I'_0=\frac{V_0}{Z'}=\frac{V_0}{2R}=\frac{I_0}{\sqrt 2}$$
  • Question 9
    1 / -0
    A coil has an inductance of $$0.7\space H$$ and is joined in series with a resistance of $$220\Omega$$. When an alternating emf of $$220\space V$$ at $$50\space cps$$ is applied to it, then the wattless component of the current in the circuit is (take $$0.7\pi = 2.2)$$
    Solution
    wattless current = $$ { I }_{ max }sin({ tan }^{ -1 }\{ L\omega /R\} )=\frac { 220 }{ \sqrt { { R }^{ 2 }+{ L }^{ 2 }{ \omega  }^{ 2 } }  } sin({ tan }^{ -1 }\{ L\omega /R\} )=0.5A $$
  • Question 10
    1 / -0
    A resistor and an inductor are connected to an ac supply of $$120\space V$$ and $$50\space Hz$$. The current in the circuit is $$3\space A$$. If the power consumed in the circuit is $$108\space W$$, then the resistance in the circuit is
    Solution
    $$ I_{rms}= current in circuit = 3A $$
    $$ P = 108 W = {I}_{rms}^{2} R =3^2 R$$
    $$ R =108/9= 12 \Omega $$
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