ALTERNATING CURRENT

This chapter discusses alternating current (AC), its properties, behavior in different circuit components, the significance of RMS values, phasor representation, and the operation of transformers in voltage transformation.

Notes on Alternating Current

7.1 Introduction to Alternating Current (AC)

  • Definition: Alternating current (AC) is an electric current that reverses direction periodically, unlike direct current (DC), which flows only in one direction.
  • Sine Wave: AC voltage is commonly represented by a sine wave function, such as v(t) = v_m sin(ωt), where:
    • v_m is the peak voltage.
    • ω is the angular frequency.
  • Importance of AC: Most electrical devices operate on AC due to its efficient transmission over long distances and ease of voltage transformation using transformers.

7.2 AC Voltage Applied to a Resistor

  • Current through Resistor: When an AC voltage is applied across a resistor, the current also varies sinusoidally: [ i(t) = i_m ext{sin}(ωt) ] Where i_m = v_m/R, following Ohm’s Law (which holds for both AC and DC).
  • In-Phase Relationship: The voltage and current in a pure resistor are in phase: their peaks, zeros, and minima occur simultaneously.
  • Average Current: The average current over a complete cycle is zero, but the average power is not:
    • Instantaneous power calculation: [ p = i^2 R ] leads to average power being positive due to averaging ( i^2 ) (it’s non-negative).

7.3 Phasor Representation

  • Phasors: Phasors are rotating vectors used to represent AC voltage and current, making it easier to analyze phase relationships and magnitudes in AC circuits.
  • Voltage and Current Phasors: In resistive circuits, voltage and current phasors are aligned, illustrating their in-phase nature.

7.4 AC Voltage Applied to an Inductor

  • Inductive Circuit Behavior: For a purely inductive circuit:
    • The current lags the voltage by 90 degrees (π/2).
    • Inductive reactance (X_L) is defined as X_L = ωL.
  • Zero Average Power: The average power consumed in a purely inductive circuit over one cycle is zero, as the energy oscillates back and forth between the source and the inductor.

7.5 AC Voltage Applied to a Capacitor

  • Capacitive Circuit Behavior: In a pure capacitive circuit:
    • The current leads the voltage by 90 degrees (π/2).
    • The capacitive reactance is defined as X_C = 1/(ωC).
  • Average Power: Similar to inductors, the average power consumed over a complete cycle is zero.

7.6 Series LCR Circuit Analysis

  • Impedance: Defined as Z = R^2 + (X_L - X_C)^2.
    • The phase angle θ between the voltage across the source and current in the circuit can be expressed as [ an(θ) = \frac{X_L - X_C}{R} ].
  • Power Factor: The power factor is cos(θ) and defines how effectively the circuit converts electric energy into work.
  • Resonance: A series RLC circuit reaches maximum current amplitude at the resonant frequency where X_L = X_C.

7.7 Transformers

  • Basic Operation: A transformer consists of two coils (primary and secondary) wrapped around a magnetic core. By electromagnetic induction, voltage can be stepped up or down between the coils.
  • Voltage and Current Relationships: The relationships between primary and secondary voltages and currents are given by:
    • [ \frac{V_s}{V_p} = \frac{N_s}{N_p} ]
    • [ \frac{I_s}{I_p} = \frac{N_p}{N_s} ] Where N_p and N_s are the number of turns in the primary and secondary coils, respectively.
  • Real-World Applications: In power distribution, transformers step up voltages for transmission to reduce energy losses over long distances.

Summary Points

  1. AC vs. DC: AC changes direction periodically, while DC flows in one direction.
  2. Sine Wave Voltage: AC voltage follows a sine wave pattern, essential for practical applications.
  3. RMS Values: The root mean square values are used to represent AC voltages and currents effectively.
  4. Phasor Diagrams: Employed to visualize phase relationships in AC circuits.
  5. Inductive Reactance: Defined as X_L = ωL, with current lagging behind the voltage by 90 degrees.
  6. Capacitive Reactance: Defined as X_C = 1/(ωC), with current leading the voltage by 90 degrees.
  7. Impedance in LCR Circuits: Z = R^2 + (X_L - X_C)^2 calculates the total opposition in AC circuits with resistive, inductive, and capacitive elements.
  8. Power Factor: Measures the efficiency of the circuit (cos(θ)).
  9. Resonance: Achieved when the inductive reactance equals the capacitive reactance, maximizing current flow.
  10. Transformers: Used to change AC voltage levels efficiently for power distribution without violating energy conservation laws.

Key terms/Concepts

1. AC vs. DC: AC fluctuates and can change direction, while DC is constant. 2. Voltage Representation: AC voltage is often depicted by a sine wave function. 3. RMS Values: The root mean square (RMS) allows comparison of AC with DC. 4. Phasors: Phasor diagrams facilitate analysis of AC circuits' phase relationships. 5. Inductive Behavior: Current in an inductor lags voltage by π/2; average power over a cycle is zero. 6. Capacitive Behavior: Current in a capacitor leads voltage by π/2; average power over a cycle is zero. 7. Impedance Formula: Total impedance in an LCR circuit is represented by: Z = √(R² + (X_L - X_C)²). 8. Power Factor: Cosine of the phase angle indicates how effectively the circuit uses electric power. 9. Resonance in RLC Circuits: Occurs when inductive and capacitive reactances are equal, maximizing current. 10. Transformers: Critical for voltage adjustments in power distribution, allowing efficient transmission.

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