Key Points

Alternating Current

14 Sections
  • Alternating Voltage and Current

    An alternating voltage is represented by v=vmsin(ωt)v = v_m \sin(\omega t) and the current by i=imsin(ωt+ϕ)i = i_m \sin(\omega t + \phi). Here, vmv_m and imi_m are the peak values, ω\omega is the angular frequency, and ϕ\phi is the phase difference.

  • RMS Voltage and Current

    The root mean square (rms) value is the effective value of AC. The rms voltage is Vrms=vm20.707vmV_{rms} = \frac{v_m}{\sqrt{2}} \approx 0.707 v_m, and the rms current is Irms=im20.707imI_{rms} = \frac{i_m}{\sqrt{2}} \approx 0.707 i_m.

  • AC Circuit with a Resistor

    In a purely resistive AC circuit, the voltage and current are in the same phase (ϕ=0\phi = 0). The relationship between peak values is given by Ohm's law, vm=imRv_m = i_m R.

  • AC Circuit with an Inductor

    In a purely inductive circuit, the current lags behind the voltage by a phase angle of π2\frac{\pi}{2}. The opposition offered is the inductive reactance, XL=ωLX_L = \omega L, where ω\omega is the angular frequency.

  • AC Circuit with a Capacitor

    In a purely capacitive circuit, the current leads the voltage by a phase angle of π2\frac{\pi}{2}. The opposition offered is the capacitive reactance, XC=1ωCX_C = \frac{1}{\omega C}.

  • Phasors

    Phasors are rotating vectors used to represent AC voltage and current. The length of the phasor represents the amplitude of the quantity, and the angle between phasors represents the phase difference.

  • Series LCR Circuit: Impedance

    For a series LCR circuit, the total effective opposition to the current is called impedance, Z. It is calculated as Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}.

  • Series LCR Circuit: Phase Angle

    The phase angle ϕ\phi between the source voltage and the circuit current in a series LCR circuit is given by tanϕ=XLXCR\tan \phi = \frac{X_L - X_C}{R}.

  • Resonance in Series LCR Circuit

    Resonance occurs when inductive reactance equals capacitive reactance (XL=XCX_L = X_C). At this point, impedance is minimum (Z=RZ=R), the current is maximum, and the resonant angular frequency is ω0=1LC\omega_0 = \frac{1}{\sqrt{LC}}.

  • Power in an AC Circuit

    The average power dissipated in an AC circuit is given by P=VrmsIrmscosϕP = V_{rms} I_{rms} \cos \phi. The term cosϕ\cos \phi is known as the power factor.

  • Power Factor and Wattless Current

    The power factor cosϕ\cos \phi ranges from 0 to 1. For a purely inductive or capacitive circuit, ϕ=±π2\phi = \pm \frac{\pi}{2}, so cosϕ=0\cos \phi = 0, and the power dissipated is zero. The current in such a circuit is called wattless current.

  • Transformers

    A transformer is a device used to change AC voltage levels based on mutual induction. For an ideal transformer, the ratio of secondary to primary voltages equals the ratio of turns in their coils: VsVp=NsNp\frac{V_s}{V_p} = \frac{N_s}{N_p}.

  • Transformer Current Relation

    In an ideal transformer with 100% efficiency, the input power equals the output power (Pp=PsP_p = P_s). This leads to the current relationship IsIp=NpNs\frac{I_s}{I_p} = \frac{N_p}{N_s}.

  • Step-Up and Step-Down Transformers

    A step-up transformer increases voltage (Ns>NpN_s > N_p) but decreases current. A step-down transformer decreases voltage (Ns<NpN_s < N_p) but increases current.

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