1.3 Alternating Current Fundamentals

1. Principle of Alternating Voltage and Current Generation, Equations, and Waveforms

  • Alternating Current (AC): It is an electric current that reverses its direction periodically, as opposed to direct current (DC), where the flow of electric charge is in one direction only.

  • Generation of AC: AC is typically generated using alternators or synchronous generators, where mechanical energy (e.g., from a turbine) is converted into electrical energy. The most common method of generation is through electromagnetic induction, where a conductor moves through a magnetic field.

  • AC Waveforms: The most basic waveform for AC is a sine wave, which represents a smooth, periodic oscillation. A typical AC waveform is defined by the following parameters:

    • Peak Value (Maximum Value): The highest value of the waveform (voltage or current).

    • RMS (Root Mean Square) Value: The effective value of the waveform. For a sinusoidal AC, the RMS value is the peak value divided by √2.

    • Average Value: The average of all instantaneous values in one complete cycle, often zero for symmetric sinusoidal waveforms.

Equation for a sinusoidal AC waveform:

v(t)=Vmaxsin(ωt+ϕ)v(t) = V_{\text{max}} \sin(\omega t + \phi)

Where:

v(t)=instantaneous voltage,Vmax=peak voltage,ω=angular frequency(ω=2πf,where f is the frequency),t=time,ϕ=phase anglev(t) = \text{instantaneous voltage}, \\ V_{\text{max}} = \text{peak voltage}, \\ \omega = \text{angular frequency} \quad (\omega = 2\pi f, \text{where } f \text{ is the frequency}), \\ t = \text{time}, \\ \phi = \text{phase angle}

2. Average, Peak, and RMS Values

  1. Peak Value:

    • The peak value (also known as the maximum value) is the highest point reached by the voltage or current in one cycle.

    • For a sinusoidal AC, the peak value is denoted as (Vpeak)( V_{\text{peak}} ) or (Ipeak)( I_{\text{peak}} ).

  2. RMS (Root Mean Square) Value:

    • The RMS value is a measure of the effective value of an AC waveform. It is the equivalent DC value that would produce the same power dissipation in a resistive load.

    • For a sinusoidal waveform:

      VRMS=Vpeak2V_{\text{RMS}} = \frac{V_{\text{peak}}}{\sqrt{2}}
    • This means that the RMS value is approximately 0.707 times the peak value for a sinusoidal waveform.

  3. Average Value:

    • The average value is the arithmetic mean of the values of the waveform over one complete cycle. For a pure sinusoidal waveform, the average value is zero (due to the symmetrical nature of the waveform). However, the average absolute value (or the rectified average value) is often used:

      Vavg=2πVpeak0.637×VpeakV_{\text{avg}} = \frac{2}{\pi} V_{\text{peak}} \approx 0.637 \times V_{\text{peak}}
    • For half-wave rectified signals, the average value is non-zero.


3. Three-Phase Systems

  • Three-Phase Power: This is a method used to generate and distribute alternating current. In a three-phase system, three conductors carry three sinusoidal voltages or currents that are out of phase with each other by (120)( 120^\circ ). It is the most common method for industrial and commercial power distribution.

  • Advantages of Three-Phase Systems:

    • Constant Power: In a three-phase system, the power delivered is more constant compared to a single-phase system, which results in smoother operation of motors.

    • More Efficient: Three-phase systems are more efficient for transmitting electrical power over long distances.

    • Smaller Conductors: For the same amount of power, a three-phase system requires less conductor material than a single-phase system.

Equations for Three-Phase Systems:

For line-to-line voltage:

VL=3Vphase(line-to-line voltage)V_L = \sqrt{3} V_{\text{phase}} \quad \text{(line-to-line voltage)}

Where:

VL=line-to-line voltageVphase=phase voltage (voltage across each phase)V_L = \text{line-to-line voltage} \\ V_{\text{phase}} = \text{phase voltage (voltage across each phase)}

For power in three-phase systems:

  • Balanced Load Power:

P=3VLILcos(θ)(Balanced Load Power)P = \sqrt{3} V_L I_L \cos(\theta) \quad \text{(Balanced Load Power)}

Where:

P=total powerVL=line-to-line voltageIL=line currentθ=phase angle between voltage and currentP = \text{total power} \\ V_L = \text{line-to-line voltage} \\ I_L = \text{line current} \\ \theta = \text{phase angle between voltage and current}

  • Total Apparent Power:

S=3VLIL(Total Apparent Power)S = \sqrt{3} V_L I_L \quad \text{(Total Apparent Power)}
  • Reactive Power:

Q=3VLILsin(θ)(Reactive Power)Q = \sqrt{3} V_L I_L \sin(\theta) \quad \text{(Reactive Power)}

The key point is that in a balanced three-phase system, the sum of the instantaneous powers in all three phases is constant.


Conclusion

  • AC is an electrical current that reverses direction periodically, generated through electromagnetic induction.

  • Key AC parameters: peak value, RMS value (effective value), and average value.

  • Three-phase systems provide more constant and efficient power, requiring less conductor material compared to single-phase systems.

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