A voltage V = V0 sin ωt is applied to a series LCR circuit. Derive the expression for the average power dissipated over a cycle. Under what condition (i) no power is dissipated even though the current flows through the circuit, (ii) maximum power is dissipated in the circuit?
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Voltage V=V0sinωt is applied to an series LCR circuit. Current is I=I0sin(ωt+ϕ) I0=V0Zϕ=tan-1XC-XLR Instantaneous power supplied by the source is P=VI =(V0sinωt)×(I0sin(ωt+ϕ) =V0I02cosϕ-cos(2ωt+ϕ) The average power over a cycle is average of the two terms on the R.H.S of the above equation. The second term is time dependent; so, its average is zero. P=V0I02cosϕ =V0I022cosϕ =VIcosϕP=I2Zcosϕ is called the power factor. Case I For pure inductive circuit or pure capacitive circuit, the phase difference between current and voltage is . Therefore, no power is dissipated. This current is sometimes referred to as wattless current. Case II For power dissipated at resonance in an LCR circuit, So, maximum power is dissipated.
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Explanation:
Power factor of the circuit is given by:
cosϕ=
Z
R
=
R
2
+(ωL−
ωC
1
)
2
R
Current flowing in the circuit is given by:
I=
Z
V
I=
Z
V
o
sin(ωt)
Instantaneous real power dissipated in the circuit is:
P=I
2
R
P=
Z
2
V
o
2
sin
2
(ωt)
R
Average power dissipated in a cycle is given by:
<P>=
∫
0
2π/ω
dt
∫
0
2π/ω
Pdt
=
2Z
2
×2π/ω
V
o
2
R
∫
0
2π/ω
(1−cos(2ωt))dt
<P>=V
rms
I
rms
cos(ϕ)
(i)
No power is dissipated when P = 0
This implies cosϕ=0
ϕ=π/2
That is the circuit is purely inductive or capacitive.
(ii)
Maximum power is dissipated when P is maximum.
This implies cosϕ=1
ϕ=0
Circuit is purely resistive.
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