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Alternating Current Test - 48

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Alternating Current Test - 48
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  • Question 1
    1 / -0
    A waveform has a baseline of $$3 V$$, a duty cycle of $$20$$%, and an amplitude of $$8 V$$. The average voltage value is
    Solution
    Baseline voltage is $$3V$$ and amplitude is $$8V$$. 
    As we know duty cycle  $$ DC=\dfrac{T_H}{T_H+T_L}$$.
    In this problem it is given as $$0.20$$, thus we get
    $$0.20 = \dfrac{T_H}{T_H+T_L}$$
    $$\implies T_L=4T_H$$
    Average value of voltage  $$V_a=\dfrac{T_H\times8+T_L\times3}{T_H+T_L}=\dfrac{20}{5}=4V$$
    $$\therefore$$ Answer is A.
  • Question 2
    1 / -0
    A $$6 kHz$$ sinusoidal voltage is applied to a series RC circuit. The frequency of the voltage across the resistor is
    Solution
    Frequency of applied voltage and voltage or current accross any component are same. As we know,
     $$I=\dfrac{V}{Z}$$ and $$Z$$ has nothing to do with frequency 
    $$\implies$$ $$I$$ and $$V$$ have same frequency. 
    And also according to KVL  $$V=V_1+V_2+V_3$$  
    $$\implies$$ voltage and current across any component have same frequency i.e $$6kHz$$.
  • Question 3
    1 / -0
    A resistor and a capacitor are in series across a $$20 V$$ ac source. Circuit impedance is $$4.33 k \Omega$$. Current flow in the circuit is
    Solution
    Voltage of the source $$V = 20$$ volts
    Circuit impedance $$Z = 4.33 k\Omega = 4.33\times 10^{3}\Omega$$
    Thus current in the circuit $$I = \dfrac{V}{Z}$$
    $$\therefore$$ $$I = \dfrac{20}{4.33\times 10^3} = 4.6 \times 10^{-3} A$$
    $$\implies$$ $$I = 4.6 mA$$
  • Question 4
    1 / -0
    In a parallel RC circuit, there is $$100 mA$$ through the resistive branch and $$100 mA$$ through the capacitive branch. The total rms current is
    Solution
    Current in resistive branch $$I_r = 100 mA$$
    Current in capacitive branch $$I_c = 100 mA$$
    Thus total rms current $$I_{rms} = \sqrt{I_r^2 + I_c^2}$$
    $$\therefore$$ $$I_{rms} = \sqrt{100^2 + 100^2}$$
    $$\implies$$ $$I_{rms} = \sqrt{2} \times 100   = 141 mA$$
  • Question 5
    1 / -0
    A resistor $$R$$, an inductor $$L$$ and capacitor $$C$$ are connected in series to an oscillator of frequency $$n$$. If the resonant frequency is $${ n }_{ r }$$, then the current lags behind voltage, when
    Solution
    When reactance of inductance is more than the reactance of condenser, the current lag behind the voltage.
    Thus $$\omega L < \dfrac { 1 }{ \omega c }$$ or $$ \omega > \dfrac { 1 }{ \sqrt { LC }  }$$
    or $$ n > \dfrac { 1 }{ 2\pi \sqrt { LC }  }$$ or $$ n > { n }_{ r }$$
    $${ n }_{ r }=$$ resonant frequency
  • Question 6
    1 / -0
    The rms value of a.c. voltage with peack of $$311 V$$ is
    Solution
    Peak value of a.c. voltage, $$V_o = 311$$ volts
    The rms value of voltage, $$V_{rms} = \dfrac{V_o}{\sqrt{2}}$$
    $$\therefore$$   $$V_{rms} = \dfrac{311}{\sqrt{2}} = \dfrac{311}{1.414} = 220$$ volts
  • Question 7
    1 / -0
    The average half-cycle value of a sine wave with a $$40 V$$ peak is
    Solution
    The source voltage $$V = V_o \sin wt$$
    Average half-cycle value of sine wave $$V_{avg} = \dfrac{\int_o^{T/2} V_o \sin (wt) dt} {T/2}$$
    Or $$V_{avg} = \dfrac{V_o} {T/2} \times \int_o^{T/2} \sin wt dt$$
    Or $$V_{avg} = \dfrac{V_o} {T/2} \times \dfrac{\cos wt}{w} \bigg|^{T/2}_o$$
    Or $$V_{avg} = \dfrac{V_o} {T/2} \times \dfrac{\cos\frac{wT}{2} - 1}{w} $$
    Or $$V_{avg} = \dfrac{V_o} {T/2} \times \dfrac{-1 - 1}{w} $$
    Or $$V_{avg} = \dfrac{V_o} {\pi } \times (-2) $$
    $$\implies$$ $$|V_{avg} | = \dfrac{2V_o}{ \pi}$$
    We get $$|V_{avg}| = \dfrac{2\times 40}{\pi} = 25.48$$ volts
  • Question 8
    1 / -0
    A sine wave with an rms value of $$12 V$$ is riding on a dc level of $$18 V$$. The maximum value of the resulting waveform is
    Solution
    Rms value of voltage $$V_{rms} = 12 $$ volts
    Thus peak voltage $$V_o = \sqrt{2} V_{rms}$$
    $$\therefore$$ $$V_o = 1.414 \times 12 = 17$$ volts
    Maximum value of resulting waveform $$V_{max} = V_o + 18$$
    $$\implies$$ $$V_{max} = 17+18 = 35$$ volts
  • Question 9
    1 / -0
    The instantaneous emf and current equations of an RLC series circuit are
    $$e=200\sin { \left( \omega t-\dfrac { \pi  }{ 6 }  \right)  } $$
    $$i=20\sin { \left( \omega t+\dfrac { \pi  }{ 6 }  \right)  } $$
    The average power consumed per cycle is
    Solution
    Instantaneous power of the circuit, $$P=ei$$
    Hence the average power of the circuit $$=\dfrac{\int_0^{2\pi/\omega} Pdt}{2\pi/\omega}$$ $$=\dfrac{\int_0^{2\pi/\omega}4000sin(\omega t-\dfrac{\pi}{6})sin(\omega t+\dfrac{\pi}{6})}{2\pi/\omega}W$$

    Using: $$cosA-cosB=-2sin(\dfrac{A+B}{2})sin(\dfrac{A-B}{2})$$

    Average power $$=\dfrac{\int_0^{2\pi/\omega}4000\dfrac{1}{2}(cos\dfrac{\pi}{3}-cos2\omega t)dt}{2\pi/\omega}W$$ $$=1000\ W$$
  • Question 10
    1 / -0
    An LC resonant circuit contains a capacitor $$400 pF$$ and an inductor $$100 \mu H$$. It is set into oscillations coupled to an antenna. Calculate the wavelength of the radiated electromagnetic wave.
    Solution
    Wavelength $$ =\lambda = \dfrac{Velocity}{Frequency} $$

    Frequency of the Resonating LC circuit = $$ \dfrac{1}{2\pi \times \sqrt {LC}} $$

    $$ \implies Wavelength =  C\times 2 \pi \times \sqrt { LC } $$

      $$=3\times { 10 }^{ 8 }\times 2\times 3.14\times \sqrt { 100\times { 10 }^{ -6 }\times 400\times { 10 }^{ -12 } } $$
      $$=376.8 m$$
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