CHPTR 31 Notes: AC Circuits

Generators and Energy Conversion

  • Generators convert mechanical energy into electrical energy.

  • An alternating current (AC) generator is depicted.

AC and DC Currents

  • Devices such as light bulbs and toasters operate effectively on both AC and direct current (DC).

  • Motors can be more easily adapted to operate with AC currents than with DC.

Circuit Symbols and Time Varying Voltages

  • The circuit symbol for an AC source is presented.

  • The time-varying voltage is defined mathematically as:
      - V(t)=Vimesextcos(heta)V(t) = V imes ext{cos}( heta) where heta=extωtheta = ext{ω}t.

  • In the U.S., the frequency of AC is given as f=60extHzf = 60 ext{Hz} which corresponds to angular frequency extω=377extrad/sext{ω} = 377 ext{rad/s}.

  • Here, VV represents the "voltage amplitude" or peak voltage.

Root Mean Square (RMS) Values

  • The root-mean-square (rms) value of sinusoidal voltage is given by:
      - Vrms=racVext2V_{rms} = rac{V}{ ext{√2}}.

  • The rms value of sinusoidal current is defined as:
      - Irms=racIext2I_{rms} = rac{I}{ ext{√2}}.

  • Therefore, for a specification of 120 volts AC, the rms voltage Vrms=120extvoltsV_{rms} = 120 ext{volts}, leading to a peak voltage amplitude V=120extVimesext2extor170extVV = 120 ext{V} imes ext{√2} ext{ or } 170 ext{V}.

Instantaneous Current and Voltage in Resistors

  • The instantaneous current I(t)I(t) and voltage V(t)V(t) across a resistor are in phase, leading to the relationships:
      - I(t)=Imaxextcos(extωt)I(t) = I_{max} ext{cos}( ext{ω}t)
      - V(t)=Vmaxextcos(extωt)V(t) = V_{max} ext{cos}( ext{ω}t)
      - Indicates that V=IimesRV = I imes R at any instant.

Inductive Reactance

  • The instantaneous voltage across an inductor is illustrated as:
      - VL=LracdidtV_L = L rac{di}{dt} and is given by:
        - VL(t)=Lextωextsin(extωt)V_L(t) = L ext{ω} ext{sin}( ext{ω}t).

  • This depicts that the voltage leads the current by 90 degrees, meaning:
      - IL(t)=Imaxextsin(extωt)I_L(t) = I_{max} ext{sin}( ext{ω}t).
      - Therefore, the relationship is captured between voltage and current as:
        - racVLIL=XL=extωLrac{V_L}{I_L} = X_L = ext{ω}L.

Capacitors and Their Reactance

  • The instantaneous current, charge, and voltage across a capacitor are given as:
      - V(t)=rac1Cimesq(t)V(t) = rac{1}{C} imes q(t), where current I(t)I(t) leads voltage by 90 degrees:
        - I(t)=Imaxextsin(extωt)I(t) = I_{max} ext{sin}( ext{ω}t),
        - V(t)=Vmaxextcos(extωt)V(t) = V_{max} ext{cos}( ext{ω}t).

  • Indicating the phase relationship:
      - extφ=90°ext{φ} = -90°.

  • The expression for capacitive reactance is:
      - XC=rac1extωCX_C = rac{1}{ ext{ω}C}.

Currents in Capacitors and Inductors

  • Current lags voltage across an inductor, represented as or recursively defined:
      - V=IXLV = IX_L.

  • Conversely, current leads voltage across a capacitor:
      - V=IXCV = IX_C.

  • Implying:
      - For a circuit, the current through each element remains the same at any given instant.

Voltage Relationships in RLC Circuits

  • For any circuit moment, the total voltage across R, L, and C combines to equal the source voltage:
      - VR+VLVC=VsV_{R} + V_{L} - V_{C} = V_{s}.

  • Voltage amplitudes related can be summarized as:
      - VR2+(VLVC)2=V2V_R^2 + (V_L - V_C)^2 = V^2.

Impedance in Series RLC Circuits

  • The impedance of a series RLC circuit is defined as:
      - Z=ext(R2+(XLXC)2)Z = ext{√}(R^2 + (X_L - X_C)^2),
        - Where the phase angle extφext{φ} is calculated as:
        - exttan(extφ)=racXLXCRext{tan}( ext{φ}) = rac{X_L - X_C}{R}.

Resonance in RLC Circuits

  • For radio signals tuned to a frequency of 101.5extkHz101.5 ext{kHz}, maximum current II is achieved when impedance ZZ is minimal:
      - V=IZV = IZ.

  • Resonance occurs when the inductive reactance equals the capacitive reactance:
      - XL=XCX_L = X_C,
      - This leads to the condition:
        - extω0L=rac1extω0Cext{ω}_0 L = rac{1}{ ext{ω}_0 C}.

  • The resonance frequency can be computed as:
      - extω0=rac1ext(LC)ext{ω}_0 = rac{1}{ ext{√(LC)}}
        - Divide this result by 2extπ2 ext{π} to convert to frequency in Hertz.

Transformers and Power Transmission

  • Losses in power transmission are minimized by transmitting at the highest possible voltages.

  • Voltage step-up and step-down transformers are utilized for efficient power transmission.

  • The voltage across the secondary coil of a transformer is defined as:
      - racV1V2=racN1N2rac{V_1}{V_2} = rac{N_1}{N_2} where N1N_1 and N2N_2 are the number of turns in the primary and secondary coils respectively.