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^LCR series or acceptor circuit

^LCR series or acceptor circuit

If the generator oscillates at a frequency equal to natural frequency of LC oscillator then current in the circuit becomes maximum & the stage is called resonance. Following points are of interest at resonance.

1. XL= XC, Z = min. = R

2.

3. Φ = 0

4. Quality factor or Q factor or voltage multiplication factor is defined as the ratio of voltage across inductor (or capacitor) VL (or VC) to ratio of voltage across a resistor at resonance. i.e.

5. Also

Here ω1 & ω2 are called half power side band frequency.

6. Value of Q describes the sharpness of I – ω curve at resonance.

If band width is low, the quality factor will be high & the I – ω graph will be thin & sharp & vice – versa as shown in the following plots. Higher the value of Q-factor, the narrower & sharper is the I – ω curve at resonance.

The larger the value of Q – factor, the smaller is the value of 2 Δω or the bandwidth and sharper is the resonance.

^Impedance triangle

^Impedance triangle

Impedance triangle is also called ac triangle.

It is obtained by the phase relationship between I & V for various elements of a given circuit & is useful to find X, R, Z, Φ, PF, Iv, Pav & WLC.

Here     X = net reactance of the circuit and R = resistance offered by the pure resistor.

^Power factor

^Power factor

Power factor is defined as, .

Its value lies between 0 & 1. To decrease the power loss in the transmission we have to increase the power factor, we can do this by making Z tend to R, for this we have to include a capacitor in the circuit.

^Wattless current

^Wattless current

The average power consumed by a pure inductor & a pure capacitor is zero while that by a pure resistor is maximum. The current flowing in a pure inductor & a pure capacitor doesn’t dissipate any power. Such a current is called wattless current or idle current. Its amount is Iv sinΦ.

^Average power consumed

^Average power consumed

Average power consumed in an ac circuit is:

Paverage = Ev Iv cosΦ

Ev Iv → is called virtual power or apparent power.

^Phase difference between I & V

^Phase difference between I & V

When ac flows through a

(a) pure R, E & I are in phase i.e. Φ = 00

(b) pure L, I  lags E by 900 i.e. Φ = + 900

(d) C, I leads E by 900 i.e Φ = – 900

The value of f for other cases depends upon the nature of circuit elements and their combinations.

^Reactance

^Reactance

Resistance offered by the L or C current in an ac circuit is called reactance. It is of two types

1. Inductive reactance XL = ωL

2. Capacitive reactance,

Inductive reactance increases with the increase in frequency of ac. An inductor offers no resistance (XL= 0) to dc, thus acts as short circuit for dc.

Capacitive reactance decreases with the increase in frequency of ac. A capacitor offers infinite resistance (XC = ∞) to dc, thus doesn’t allow dc to pass through it & acts as open circuit for dc.

^Impedance

^Impedance

Net resistance offered by the combination of L, C & R to current in an ac ckt. is called impedance (Z).

^Current in ac circuits

^Current in ac circuits

Let E = E0 sin ωt is the sinusoidal source of emf applied to a circuit. Let Φ is the phase difference between current & the emf applied is, then the current flowing through the circuit can be represented by the general relation

I = I0 sin (ωt + Φ), its virtual value of current is

Current flowing in a circuit depends upon following factors:

(a) input voltage signal

(b) frequency of the input voltage signal

(c) nature of circuit elements in the circuit

(d) combination of circuit elements in the circuit

^ac generator

^ac generator

Also called dynamos or electric oscillators or commutators is based on EMI. When a metallic – coil is rotated at a high speed in a strong magnetic field, due to the change in magnetic flux linked with the coil a voltage difference ε = ε0 sin ωt, ε0 = BANω is induced across the two ends of the coil connected to the rings R1 & R2 called Slip rings, which when fed to external load through carbon brushed B1 & B2 can supply current to load.

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