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Question: In an a.c. circuit with phase voltage \(V\) and current \(I\), the power dissipated is: A. \(\dfra...

In an a.c. circuit with phase voltage VV and current II, the power dissipated is:
A. VI2\dfrac{{VI}}{2}
B. VI2\dfrac{{VI}}{{\sqrt 2 }}
C. VIVI
D. VIcosθVI\cos \theta

Explanation

Solution

To solve this question, we will consider RLC a.c. circuit whose total impedance is Z. We will first use the relation between power, voltage, current and resistance. After that, we will use the total impedance to find the required answer.In capacitive circuit, the circuit contains only capacitor and hence the phase difference between voltage and current is 900{90^0} which means that θ=π2cosθ=0\theta = \dfrac{\pi }{2} \Rightarrow \cos \theta = 0.Thus, there is no power dissipation in the capacitive circuit.

Formulas used:
P=I2RP = {I^2}R ,
where, PP is the dissipated power dissipated, II is current and RR is resistance.
I=VZI = \dfrac{V}{Z},
where, II is current, VVis voltage and ZZ is total impedance of the circuit.
RZ=cosθ\dfrac{R}{Z} = \cos \theta ,
where, RR is resistance, ZZ is total impedance of the circuit and cosθ\cos \theta is the power factor where θ\theta is the phase difference between voltage and current.

Complete step by step answer:
We know that power dissipated is given by:
P=I2RP = {I^2}R
We can rewrite this equation as
P=IRIP = IRI
Now, we will put I=VZI = \dfrac{V}{Z}
P=IRVZP = IR\dfrac{V}{Z}
This can be rewritten as
P=IVRZP = IV\dfrac{R}{Z}
But, we know that RZ=cosθ\dfrac{R}{Z} = \cos \theta
P=IVcosθ\therefore P = IV\cos \theta
Thus power dissipated in a.c. circuit with phase voltage VVand current IIis VIcosθVI\cos \theta .

Hence, option D is the right answer.

Note: Here, we have seen that power is dependent on values of voltage and current as well as the power factor. There are two important cases: resistive circuit and capacitive circuit. In a resistive circuit, the circuit contains only pure resistance and hence there is no phase difference between voltage and current which means that θ=0cosθ=1\theta = 0 \Rightarrow \cos \theta = 1. Thus, there is maximum power dissipation in a resistive circuit.