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JEE Physics 2024 Question with Solution

A series LRL-R circuit connected to an AC source E=25sin(1000t)VE = 25 \sin(1000t) \, \text{V} has a power factor of 12\frac{1}{\sqrt{2}}. If the source of emf is changed to E=20sin(2000t)VE = 20 \sin(2000t) \, \text{V}, the new power factor of the circuit will be:

  • A

    12\frac{1}{\sqrt{2}}

  • B

    13\frac{1}{\sqrt{3}}

  • C

    15\frac{1}{\sqrt{5}}

  • D

    17\frac{1}{\sqrt{7}}

Answer

Correct answer:C

Step-by-step solution

Standard Method

Given: A series LRL-R circuit has initial source E=25sin(1000t)VE = 25 \sin(1000t) \, \text{V} and initial power factor cosϕ1=12\cos \phi_1 = \frac{1}{\sqrt{2}}. The source is changed to E=20sin(2000t)VE = 20 \sin(2000t) \, \text{V}.

Find: The new power factor of the circuit.

For a series LRL-R circuit, the power factor is

cosϕ=RZ=RR2+XL2\cos \phi = \frac{R}{Z} = \frac{R}{\sqrt{R^2 + X_L^2}}

where

XL=ωLX_L = \omega L

Initially,

ω1=1000rad/s\omega_1 = 1000 \, \text{rad/s}

and

12=RR2+(1000L)2\frac{1}{\sqrt{2}} = \frac{R}{\sqrt{R^2 + (1000L)^2}}

Squaring and simplifying gives

12=R2R2+(1000L)2\frac{1}{2} = \frac{R^2}{R^2 + (1000L)^2}

so

R2+(1000L)2=2R2R^2 + (1000L)^2 = 2R^2

Therefore,

(1000L)2=R2(1000L)^2 = R^2

which means

1000L=R1000L = R

Now the new angular frequency is

ω2=2000rad/s\omega_2 = 2000 \, \text{rad/s}

Hence the new inductive reactance becomes

XL2=2000L=2RX_{L2} = 2000L = 2R

So the new power factor is

cosϕ2=RR2+(2R)2=R5R2=15\cos \phi_2 = \frac{R}{\sqrt{R^2 + (2R)^2}} = \frac{R}{\sqrt{5R^2}} = \frac{1}{\sqrt{5}}

Therefore, the new power factor is 15\frac{1}{\sqrt{5}} and the correct option is C.

Using tan relation

Given: Initial power factor cosθ=12\cos \theta = \frac{1}{\sqrt{2}} for a series LRL-R circuit.

Find: The new power factor when angular frequency changes from 1000rad/s1000 \, \text{rad/s} to 2000rad/s2000 \, \text{rad/s}.

Since

cosθ=12\cos \theta = \frac{1}{\sqrt{2}}

we get

tanθ=1\tan \theta = 1

Hence initially,

XLR=1XL=R\frac{X_L}{R} = 1 \Rightarrow X_L = R

When frequency doubles, inductive reactance also doubles because

XL=ωLX_L = \omega L

So at the new frequency,

XL=2RX_L' = 2R

Now,

tanθ=XLR=2\tan \theta' = \frac{X_L'}{R} = 2

Therefore,

cosθ=11+tan2θ=11+4=15\cos \theta' = \frac{1}{\sqrt{1+\tan^2 \theta'}} = \frac{1}{\sqrt{1+4}} = \frac{1}{\sqrt{5}}

Therefore, the new power factor is 15\frac{1}{\sqrt{5}}.

Common mistakes

  • A common mistake is to think that changing the voltage amplitude from 25V25 \, \text{V} to 20V20 \, \text{V} changes the power factor. This is wrong because power factor in a series LRL-R circuit depends on the phase relation between RR and XLX_L, not on source amplitude. Focus on the change in angular frequency instead.

  • Students often use the initial power factor 12\frac{1}{\sqrt{2}} directly as the final answer. This is incorrect because inductive reactance changes with frequency as XL=ωLX_L = \omega L. Recalculate the reactance ratio after the frequency changes.

  • Another mistake is to assume reactance doubles but then substitute it as XL=2XLX_L = 2X_L without relating it to RR. From the initial condition, first establish that 1000L=R1000L = R or equivalently initial XL=RX_L = R, and only then compute the new reactance as 2R2R.

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