12.3 RLC circuits and resonance

RLC circuits combine resistors, inductors, and capacitors, creating complex AC behavior. These circuits showcase the interplay between resistance, inductance, and capacitance, leading to fascinating phenomena like resonance and frequency-dependent responses.

Understanding RLC circuits is crucial for grasping AC circuit analysis. They form the foundation for many real-world applications, from radio tuners to power distribution systems, and help explain how different components interact in alternating current environments.

Components in RLC Circuits

Passive Circuit Elements

Top images from around the web for Passive Circuit Elements

• 

  Ohm’s Law: Resistance and Simple Circuits | Physics View original

  Is this image relevant?

• 

  RLC Series AC Circuits | Physics View original

  Is this image relevant?

• 

  RLC circuit - Wikiversity View original

  Is this image relevant?

• 

  Ohm’s Law: Resistance and Simple Circuits | Physics View original

  Is this image relevant?

• 

  RLC Series AC Circuits | Physics View original

  Is this image relevant?

1 of 3

Top images from around the web for Passive Circuit Elements

• 

  Ohm’s Law: Resistance and Simple Circuits | Physics View original

  Is this image relevant?

• 

  RLC Series AC Circuits | Physics View original

  Is this image relevant?

• 

  RLC circuit - Wikiversity View original

  Is this image relevant?

• 

  Ohm’s Law: Resistance and Simple Circuits | Physics View original

  Is this image relevant?

• 

  RLC Series AC Circuits | Physics View original

  Is this image relevant?

1 of 3

• Resistor opposes the flow of electric current in a circuit
  • Resistance measured in ohms ($\Omega$)
  • Voltage across a resistor is proportional to the current flowing through it (Ohm's law: $V = IR$)
• Inductor stores energy in a magnetic field when electric current flows through it
  • Inductance measured in henries (H)
  • Opposes changes in current, causing a phase shift between voltage and current
  • Voltage across an inductor is proportional to the rate of change of current ($V_L = L \frac{dI}{dt}$)
• Capacitor stores energy in an electric field between two conducting plates
  • Capacitance measured in farads (F)
  • Opposes changes in voltage, causing a phase shift between voltage and current
  • Current through a capacitor is proportional to the rate of change of voltage ($I_C = C \frac{dV}{dt}$)

Impedance and Reactance

• Impedance is the total opposition to the flow of alternating current in a circuit
  • Measured in ohms ($\Omega$)
  • Consists of resistance and reactance (inductive and capacitive)
• Inductive reactance ($X_L$) is the opposition to the flow of alternating current due to the presence of an inductor
  • Increases with frequency ($X_L = 2\pi fL$)
• Capacitive reactance ($X_C$) is the opposition to the flow of alternating current due to the presence of a capacitor
  • Decreases with frequency ($X_C = \frac{1}{2\pi fC}$)

RLC Circuit Configurations

Series RLC Circuit

• Resistor, inductor, and capacitor connected in series
• Current is the same through all components
• Total voltage is the sum of the voltages across each component ($V_T = V_R + V_L + V_C$)
• Impedance is the vector sum of resistance and reactances ($Z = \sqrt{R^2 + (X_L - X_C)^2}$)
• Phase angle between voltage and current depends on the relative values of $X_L$ and $X_C$

Parallel RLC Circuit

• Resistor, inductor, and capacitor connected in parallel
• Voltage is the same across all components
• Total current is the sum of the currents through each component ($I_T = I_R + I_L + I_C$)
• Admittance (Y) is the reciprocal of impedance ($Y = \frac{1}{Z}$)
  • Measured in siemens (S)
• Phase angle between voltage and current depends on the relative values of the branch currents

Resonance Characteristics

Resonance Frequency

• Frequency at which the inductive and capacitive reactances are equal ($X_L = X_C$)
• At resonance, the impedance is purely resistive ($Z = R$)
• Maximum current in series RLC circuit and maximum voltage in parallel RLC circuit occur at resonance
• Resonance frequency ($f_0$) can be calculated using the formula: $f_0 = \frac{1}{2\pi \sqrt{LC}}$

Quality Factor

• Measure of the sharpness of the resonance peak and the selectivity of the circuit
• Defined as the ratio of the resonance frequency to the bandwidth ($Q = \frac{f_0}{\Delta f}$)
• Higher Q factor indicates a sharper resonance peak and better frequency selectivity
• In series RLC circuit, $Q = \frac{2\pi f_0 L}{R}$; in parallel RLC circuit, $Q = \frac{R}{2\pi f_0 L}$

Bandwidth

• Range of frequencies over which the power in the circuit is at least half of its maximum value
• Measured as the difference between the upper and lower half-power frequencies ($\Delta f = f_2 - f_1$)
• Half-power frequencies are the points where the power in the circuit is half of its maximum value
  • Occurs when the impedance is $\sqrt{2}$ times the minimum impedance
• Narrower bandwidth indicates better frequency selectivity and higher Q factor