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Online simulation of the переменный ток circuit

Shown here is a classic alternating-current circuit with passive elements connected in series

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This is a simple single-diode AC rectifier circuit (a half-wave rectifier). 

What we have here

  1. AC voltage source (on the left)

    • Frequency: 131 Hz

    • Amplitude: about ±6 V

    • The signal is sinusoidal (an up-and-down wave)

  2. Light source (red LED)(in the center)

    • Passes current in only one direction

  3. 35 Ω resistor (the load)

    • Current flows through it

    • The output voltage is taken across it

  4. Output (on the right)

    • This is the voltage across the resistor

 How the circuit works

 When the input wave is positive

  • The diode opens (passes current)

  • Current flows through the resistor to ground

  • A voltage appears at the output (the green "hump")

 When the wave is negative

  • The diode closes

  • No current flows

  • The output voltage = 0

 What you can see on the graphs

  • On the left (input) — an ordinary sine wave

  • On the right (output) — only the upper halves of the sine wave

 This is exactly half-wave rectification

Why the output is lower (≈3.97 V — this is an instantaneous value, not 6 V)

Because:

  • The diode "eats up" ~0.7 V (the voltage drop)

  • And some energy is lost

 

Input: a sine wave with amplitude

Uin(max)=6 ВU_{in(max)} = 6\text{ В}

There is a diode (voltage drop of about 0.7 V)

Load: a resistor (it has almost no effect on the waveform)

 Accounting for the diode drop

When the diode is open:

Uout=UinUdU_{out} = U_{in} - U_{d}

Where:

  • Ud0.7 ВU_d \approx 0.7\text{ В}

Then the maximum value:

Uout(max)=60.7=5.3 ВU_{out(max)} = 6 - 0.7 = 5.3\text{ В}

 Summary

The circuit does the following:

It converts alternating current into pulsating direct current, passing only the positive part of the signal.


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