MHT CET · Maths · Differential Equations
The particular solution of the differential equation \(\left(1+e^{2 x}\right) d y+e^x\left(1+y^2\right) d x=0\) at \(x=0\) and \(y=1\) is
- A \(\tan ^{-1} \mathrm{e}^{\mathrm{x}}-\tan ^{-1} \mathrm{y}=0\)
- B \(\tan ^{-1} \mathrm{e}^{\mathrm{x}}+\tan ^{-1} \mathrm{y}=\frac{\pi}{2}\)
- C \(\tan ^{-1} \mathrm{e}^{\mathrm{x}}+\tan ^{-1} \mathrm{y}=\frac{3 \pi}{4}\)
- D \(\tan ^{-1} e^x-\tan ^{-1} y=\frac{3 \pi}{4}\)
Answer & Solution
Correct Answer
(B) \(\tan ^{-1} \mathrm{e}^{\mathrm{x}}+\tan ^{-1} \mathrm{y}=\frac{\pi}{2}\)
Step-by-step Solution
Detailed explanation
\(\begin{aligned}
& \left(1+\mathrm{e}^{2 \mathrm{x}}\right) \mathrm{dy}+\mathrm{e}^{\mathrm{x}}\left(1+\mathrm{y}^2\right) \mathrm{dx}=0 \\
& \therefore \frac{\mathrm{dy}}{1+\mathrm{y}^2}+\frac{\mathrm{e}^{\mathrm{x}}}{\left(1+\mathrm{e}^{2 \mathrm{x}}\right)} \mathrm{dx}=0 \\
& \therefore \int \frac{\mathrm{dy}}{1+\mathrm{y}^2}=-\int \frac{\mathrm{e}^{\mathrm{x}}}{1+\mathrm{e}^{2 \mathrm{x}}} d \mathrm{x}
\end{aligned}\)
Put \(\mathrm{e}^{\mathrm{x}}=\mathrm{t} \Rightarrow \mathrm{e}^{\mathrm{x}} \mathrm{dx}=\mathrm{dt}\)
\(\therefore \int \frac{\mathrm{dy}}{1+\mathrm{y}^2}=-\int \frac{\mathrm{dt}}{1+\mathrm{t}^2} \Rightarrow \tan ^{-1}(\mathrm{y})=-\tan ^{-1}(\mathrm{t})+\mathrm{c}\)
\(\therefore \tan ^{-1}(\mathrm{y})+\tan ^{-1}\left(\mathrm{e}^{\mathrm{x}}\right)=\mathrm{c}\)
We have \(\mathrm{x}=0, \mathrm{y}=1\)
\(\therefore \tan ^{-1}(1)+\tan ^{-1}\left(\mathrm{e}^{\circ}\right)=\mathrm{c} \Rightarrow \mathrm{c}=2 \tan ^{-1}(1)=\frac{\pi}{2}\)
\(\therefore \tan ^{-1} \mathrm{y}+\tan ^{-1} \mathrm{e}^{\mathrm{x}}=\frac{\pi}{2}\)
& \left(1+\mathrm{e}^{2 \mathrm{x}}\right) \mathrm{dy}+\mathrm{e}^{\mathrm{x}}\left(1+\mathrm{y}^2\right) \mathrm{dx}=0 \\
& \therefore \frac{\mathrm{dy}}{1+\mathrm{y}^2}+\frac{\mathrm{e}^{\mathrm{x}}}{\left(1+\mathrm{e}^{2 \mathrm{x}}\right)} \mathrm{dx}=0 \\
& \therefore \int \frac{\mathrm{dy}}{1+\mathrm{y}^2}=-\int \frac{\mathrm{e}^{\mathrm{x}}}{1+\mathrm{e}^{2 \mathrm{x}}} d \mathrm{x}
\end{aligned}\)
Put \(\mathrm{e}^{\mathrm{x}}=\mathrm{t} \Rightarrow \mathrm{e}^{\mathrm{x}} \mathrm{dx}=\mathrm{dt}\)
\(\therefore \int \frac{\mathrm{dy}}{1+\mathrm{y}^2}=-\int \frac{\mathrm{dt}}{1+\mathrm{t}^2} \Rightarrow \tan ^{-1}(\mathrm{y})=-\tan ^{-1}(\mathrm{t})+\mathrm{c}\)
\(\therefore \tan ^{-1}(\mathrm{y})+\tan ^{-1}\left(\mathrm{e}^{\mathrm{x}}\right)=\mathrm{c}\)
We have \(\mathrm{x}=0, \mathrm{y}=1\)
\(\therefore \tan ^{-1}(1)+\tan ^{-1}\left(\mathrm{e}^{\circ}\right)=\mathrm{c} \Rightarrow \mathrm{c}=2 \tan ^{-1}(1)=\frac{\pi}{2}\)
\(\therefore \tan ^{-1} \mathrm{y}+\tan ^{-1} \mathrm{e}^{\mathrm{x}}=\frac{\pi}{2}\)
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