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Identify the circuit type and output waveform.

Physics

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Step-by-step solution

4 steps

To find the average value of the output voltage, we first need to analyze the circuit.

  1. Identify the circuit type and output waveform.

    The circuit shown is a half-wave rectifier. The input voltage is vi=Vmsin⁡(ωt)v_i = V_m \sin(\omega t).

    • During the positive half-cycle of the input voltage (0≤t≤T/20 \le t \le T/2), the diode is forward-biased (assuming an ideal diode with 0V drop). Thus, the output voltage vov_o is equal to the input voltage viv_i. vo(t)=Vmsin⁡(ωt)for 0≤t≤T/2v_o(t) = V_m \sin(\omega t) \quad \text{for } 0 \le t \le T/2
    • During the negative half-cycle of the input voltage (T/2<t≤TT/2 < t \le T), the diode is reverse-biased. It acts as an open circuit, so no current flows through the resistor RR. Therefore, the output voltage vov_o is 0. vo(t)=0for T/2<t≤Tv_o(t) = 0 \quad \text{for } T/2 < t \le T
  2. Calculate the average value of the output voltage.

    The average value of a periodic waveform vo(t)v_o(t) over one period TT is given by the formula:

    Vavg=1T∫0Tvo(t) dtV_{avg} = \frac{1}{T} \int_0^T v_o(t)\,dt

    Substitute the output voltage waveform into the integral:

    Vavg=1T[∫0T/2Vmsin⁡(ωt) dt+∫T/2T0 dt]V_{avg} = \frac{1}{T} \left[ \int_0^{T/2} V_m \sin(\omega t)\,dt + \int_{T/2}^T 0\,dt \right] Vavg=1T∫0T/2Vmsin⁡(ωt) dtV_{avg} = \frac{1}{T} \int_0^{T/2} V_m \sin(\omega t)\,dt
  3. Perform the integration.

    We know that ω=2πT\omega = \frac{2\pi}{T}.

    Vavg=VmT[−cos⁡(ωt)ω]0T/2V_{avg} = \frac{V_m}{T} \left[ -\frac{\cos(\omega t)}{\omega} \right]_0^{T/2} Vavg=−VmωT[cos⁡(ωT2)−cos⁡(0)]V_{avg} = -\frac{V_m}{\omega T} \left[ \cos\left(\omega \frac{T}{2}\right) - \cos(0) \right]

    Substitute ωT=2π\omega T = 2\pi:

    Vavg=−Vm2π[cos⁡(2πTT2)−cos⁡(0)]V_{avg} = -\frac{V_m}{2\pi} \left[ \cos\left(\frac{2\pi}{T} \frac{T}{2}\right) - \cos(0) \right] Vavg=−Vm2π[cos⁡(π)−cos⁡(0)]V_{avg} = -\frac{V_m}{2\pi} \left[ \cos(\pi) - \cos(0) \right] Vavg=−Vm2π[−1−1]V_{avg} = -\frac{V_m}{2\pi} \left[ -1 - 1 \right] Vavg=−Vm2π(−2)V_{avg} = -\frac{V_m}{2\pi} (-2) Vavg=2Vm2πV_{avg} = \frac{2V_m}{2\pi} Vavg=VmπV_{avg} = \frac{V_m}{\pi}
  4. Convert to decimal value.

    Using the approximation π≈3.14159\pi \approx 3.14159:

    Vavg≈13.14159Vm≈0.3183VmV_{avg} \approx \frac{1}{3.14159} V_m \approx 0.3183 V_m

    Comparing this result with the given options:
    A) VmV_m
    B) 0.5Vm0.5V_m
    C) 0.318Vm0.318V_m
    D) 0.636Vm0.636V_m

    The calculated average value matches option C.

    The final answer is C\boxed{\text{C}}.

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