MHT CET · Physics · Alternating Current
The power factor of an R-L circuit is \(\frac{1}{\sqrt{2}}\). If the frequency of \(\mathrm{AC}\) is doubled the power factor will now be
- A \(\frac{1}{\sqrt{3}}\)
- B \(\frac{1}{\sqrt{5}}\)
- C \(\frac{1}{\sqrt{7}}\)
- D \(\frac{1}{\sqrt{11}}\)
Answer & Solution
Correct Answer
(B) \(\frac{1}{\sqrt{5}}\)
Step-by-step Solution
Detailed explanation
The power factor of an R-L circuit is given as,
\(\begin{aligned}
& \quad \cos \phi=\frac{\mathrm{R}}{\sqrt{\mathrm{R}^2+\mathrm{X}_{\mathrm{L}}{ }^2}} \\
& \therefore \quad \frac{\mathrm{R}}{\sqrt{\mathrm{R}^2+\mathrm{X}_{\mathrm{L}}{ }^2}}=\frac{1}{\sqrt{2}} \\
& \therefore \quad \frac{1}{\sqrt{1+\left(\frac{\mathrm{X}_{\mathrm{L}}}{\mathrm{R}}\right)^2}}=\frac{1}{\sqrt{2}} \\
& \therefore \quad \frac{1}{\sqrt{1+\left(\frac{\omega \mathrm{L}}{\mathrm{R}}\right)^2}}=\frac{1}{\sqrt{2}} \\
& \therefore \quad\left(\frac{\omega \mathrm{L}}{\mathrm{R}}\right)^2+1=2 \\
& \therefore \quad \frac{\omega \mathrm{L}}{\mathrm{R}}=1
\end{aligned}\)
So, when the AC frequency is doubled,
\(\begin{aligned}
\frac{\omega \mathrm{L}}{\mathrm{R}} & =2 \\
\therefore \quad \cos \phi & =\frac{1}{\sqrt{1+\left(\frac{\omega \mathrm{L}}{\mathrm{R}}\right)^2}}=\frac{1}{\sqrt{1+(2)^2}} \\
\therefore \quad \cos \phi & =\frac{1}{\sqrt{5}}
\end{aligned}\)
\(\begin{aligned}
& \quad \cos \phi=\frac{\mathrm{R}}{\sqrt{\mathrm{R}^2+\mathrm{X}_{\mathrm{L}}{ }^2}} \\
& \therefore \quad \frac{\mathrm{R}}{\sqrt{\mathrm{R}^2+\mathrm{X}_{\mathrm{L}}{ }^2}}=\frac{1}{\sqrt{2}} \\
& \therefore \quad \frac{1}{\sqrt{1+\left(\frac{\mathrm{X}_{\mathrm{L}}}{\mathrm{R}}\right)^2}}=\frac{1}{\sqrt{2}} \\
& \therefore \quad \frac{1}{\sqrt{1+\left(\frac{\omega \mathrm{L}}{\mathrm{R}}\right)^2}}=\frac{1}{\sqrt{2}} \\
& \therefore \quad\left(\frac{\omega \mathrm{L}}{\mathrm{R}}\right)^2+1=2 \\
& \therefore \quad \frac{\omega \mathrm{L}}{\mathrm{R}}=1
\end{aligned}\)
So, when the AC frequency is doubled,
\(\begin{aligned}
\frac{\omega \mathrm{L}}{\mathrm{R}} & =2 \\
\therefore \quad \cos \phi & =\frac{1}{\sqrt{1+\left(\frac{\omega \mathrm{L}}{\mathrm{R}}\right)^2}}=\frac{1}{\sqrt{1+(2)^2}} \\
\therefore \quad \cos \phi & =\frac{1}{\sqrt{5}}
\end{aligned}\)
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