🧲Electromagnetism I Unit 12 – AC Circuits and Phasors

Fundamentals of AC Circuits

• AC circuits involve time-varying currents and voltages that periodically change direction and magnitude
• Alternating current (AC) flows back and forth in a circuit, while direct current (DC) flows in only one direction
• AC is generated by devices such as alternators and is used in power distribution systems due to its ability to be easily transformed to different voltage levels
• AC circuits can include resistors, capacitors, and inductors, which affect the behavior of the current and voltage in the circuit
• The frequency of an AC signal represents the number of cycles per second and is measured in hertz (Hz)
• In the United States, the standard frequency for AC power distribution is 60 Hz, while in many other countries, it is 50 Hz
• AC circuits can be analyzed using techniques such as phasor analysis and complex impedance, which simplify calculations by representing sinusoidal waveforms as vectors

Sinusoidal Waveforms and Frequency

• Sinusoidal waveforms are the most common type of AC signal and are characterized by a smooth, periodic oscillation
• The amplitude of a sinusoidal waveform represents the maximum value of the signal and is typically measured in volts or amperes
• The period of a sinusoidal waveform is the time required for one complete cycle and is measured in seconds
  • The period is the reciprocal of the frequency: $T = \frac{1}{f}$
• The phase of a sinusoidal waveform describes the position of the wave relative to a reference point and is typically measured in degrees or radians
• Sinusoidal waveforms can be represented mathematically using the equation: $v(t) = V_m \sin(2\pi ft + \phi)$, where $V_m$ is the amplitude, $f$ is the frequency, $t$ is time, and $\phi$ is the phase angle
• The root mean square (RMS) value of a sinusoidal waveform is the equivalent DC value that would produce the same average power in a resistive load
  • For a pure sinusoidal waveform, the RMS value is equal to the amplitude divided by $\sqrt{2}$: $V_{RMS} = \frac{V_m}{\sqrt{2}}$
• Sinusoidal waveforms can be combined using the principle of superposition to create more complex waveforms

Introduction to Phasors

• Phasors are complex numbers that represent sinusoidal waveforms in the frequency domain
• Phasors simplify AC circuit analysis by eliminating the need to work with time-varying functions
• A phasor is represented by a magnitude and an angle, with the magnitude corresponding to the amplitude of the sinusoidal waveform and the angle representing the phase shift
• Phasors can be expressed in rectangular form $(a + jb)$ or polar form $(A \angle \theta)$, where $A$ is the magnitude and $\theta$ is the angle
• Phasor addition and subtraction can be performed by adding or subtracting the real and imaginary components separately
• Phasor multiplication and division involve multiplying or dividing the magnitudes and adding or subtracting the angles
• Kirchhoff's voltage and current laws can be applied to phasor quantities in AC circuits, simplifying the analysis process

Impedance and Reactance

• Impedance is a measure of the opposition to current flow in an AC circuit and is represented by the complex quantity $Z = R + jX$, where $R$ is the resistance and $X$ is the reactance
• Resistance is the real part of impedance and represents the opposition to current flow due to the dissipation of energy as heat
• Reactance is the imaginary part of impedance and represents the opposition to current flow due to the storage of energy in capacitors and inductors
  • Capacitive reactance is given by $X_C = \frac{1}{2\pi fC}$, where $f$ is the frequency and $C$ is the capacitance
  • Inductive reactance is given by $X_L = 2\pi fL$, where $f$ is the frequency and $L$ is the inductance
• The magnitude of impedance is given by $|Z| = \sqrt{R^2 + X^2}$, and the phase angle is given by $\theta = \tan^{-1}(\frac{X}{R})$
• In a purely resistive circuit, the current and voltage are in phase, while in a purely reactive circuit, the current and voltage are 90° out of phase
• The impedance of a circuit determines the relationship between the voltage and current phasors, with $V = IZ$

AC Circuit Analysis Techniques

• Nodal analysis involves applying Kirchhoff's current law (KCL) to each node in an AC circuit and solving for the node voltages using phasor quantities
• Mesh analysis involves applying Kirchhoff's voltage law (KVL) to each mesh in an AC circuit and solving for the mesh currents using phasor quantities
• Superposition theorem states that the response of a linear AC circuit to multiple sources can be found by calculating the response to each source individually and then summing the results
• Thevenin's theorem allows a complex AC circuit to be reduced to an equivalent circuit consisting of a single voltage source and a series impedance
  • The Thevenin equivalent voltage is the open-circuit voltage at the terminals of interest
  • The Thevenin equivalent impedance is the impedance seen from the terminals of interest when all sources are replaced by their internal impedances
• Norton's theorem is similar to Thevenin's theorem but uses a current source and a parallel impedance
  • The Norton equivalent current is the short-circuit current at the terminals of interest
  • The Norton equivalent impedance is the same as the Thevenin equivalent impedance
• Maximum power transfer theorem states that a load receives maximum power when its impedance is equal to the complex conjugate of the source impedance

Power in AC Circuits

• In AC circuits, power consists of three components: real power (P), reactive power (Q), and apparent power (S)
• Real power, measured in watts (W), represents the average power consumed by resistive elements and is given by $P = V_{RMS}I_{RMS}\cos(\theta)$, where $\theta$ is the phase angle between the voltage and current
• Reactive power, measured in volt-ampere reactive (VAR), represents the power stored and released by capacitive and inductive elements and is given by $Q = V_{RMS}I_{RMS}\sin(\theta)$
• Apparent power, measured in volt-ampere (VA), is the product of the RMS voltage and RMS current and represents the total power supplied to the circuit: $S = V_{RMS}I_{RMS}$
• The relationship between real, reactive, and apparent power is given by the power triangle: $S^2 = P^2 + Q^2$
• Power factor (PF) is the ratio of real power to apparent power and represents the efficiency of power utilization in an AC circuit: $PF = \frac{P}{S} = \cos(\theta)$
• A power factor of 1 indicates that all the power supplied to the circuit is consumed by resistive elements, while a power factor less than 1 indicates the presence of reactive elements
• Power factor correction can be achieved by adding capacitors or inductors to the circuit to compensate for the reactive power and improve the power factor

Resonance in AC Circuits

• Resonance occurs in an AC circuit when the inductive and capacitive reactances are equal in magnitude, resulting in a purely resistive impedance
• At resonance, the impedance of the circuit is minimized, and the current flow is maximized
• Series resonance occurs when a capacitor and inductor are connected in series, and the resonant frequency is given by $f_r = \frac{1}{2\pi\sqrt{LC}}$
  • At series resonance, the impedance is equal to the resistance, and the current is in phase with the voltage
• Parallel resonance occurs when a capacitor and inductor are connected in parallel, and the resonant frequency is the same as for series resonance
  • At parallel resonance, the impedance is maximized, and the current is minimized
• The quality factor (Q) of a resonant circuit is a measure of its selectivity and is given by $Q = \frac{f_r}{\Delta f}$, where $\Delta f$ is the bandwidth
  • A higher Q indicates a more selective circuit with a narrower bandwidth
• Resonant circuits are used in various applications, such as filters, oscillators, and tuned amplifiers, to select or reject specific frequencies

Applications and Real-World Examples

• AC power distribution systems use transformers to step up the voltage for long-distance transmission and step down the voltage for local distribution and consumption
• Household appliances, such as refrigerators, air conditioners, and washing machines, operate on AC power and contain motors, compressors, and other inductive and capacitive elements
• Electronic devices, such as smartphones, laptops, and televisions, use AC adapters or power supplies to convert AC power from the wall outlet to the appropriate DC voltage for the device
• Induction cooktops use the principles of electromagnetic induction to generate heat in the cookware, providing a more efficient and safer cooking method compared to traditional electric or gas stoves
• Wireless power transfer systems, such as those used for charging electric vehicles or mobile devices, rely on resonant coupling between coils to transfer power efficiently over short distances
• Audio and video equipment, such as speakers, microphones, and cameras, often incorporate AC circuits and resonant elements to process and filter signals
• Lighting systems, including fluorescent and LED lamps, use AC power and may include ballasts or drivers to regulate the current and provide the appropriate voltage for optimal performance
• Electric motors, found in various industrial and transportation applications, use AC power and rely on the interaction between magnetic fields and currents to generate torque and motion