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Differential Equations question

2024 · 31 Jan · Shift 2 · Q52
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  5. /2024 · 31 Jan · Shift 2 · Q52

Differential Equations question

2024 · 31 Jan · Shift 2 · Q52

JEE MainMathematicsDifferential EquationsNumerical+4 / −1
Let y=y(x)y=y(x)y=y(x) be the solution of the differential equation sec⁡2xdx+(e2ytan⁡2x+tan⁡x)dy=0,0<x<π2,y(π/4)=0\sec ^2 x d x+\left(e^{2 y} \tan ^2 x+\tan x\right) d y=0,0\lt x\lt \frac{\pi}{2}, y(\pi / 4)=0sec2xdx+(e2ytan2x+tanx)dy=0,0<x<2π​,y(π/4)=0. If y(π/6)=αy(\pi / 6)=\alphay(π/6)=α, then e8αe^{8 \alpha}e8α is equal to ‾\underline{\hspace{2cm}}​.
Numerical answer
View written solutionFree

Correct answer: 9

  1. Given differential equation
sec⁡2x dx+(e2ytan⁡2x+tan⁡x)dy=0\sec^2 x\,dx+\left(e^{2y}\tan^2 x+\tan x\right)dy=0sec2xdx+(e2ytan2x+tanx)dy=0

with

0<x<π2,y(π4)=00<x<\frac{\pi}{2}, \qquad y\left(\frac{\pi}{4}\right)=00<x<2π​,y(4π​)=0

We need to find α=y(π6)\alpha=y\left(\frac{\pi}{6}\right)α=y(6π​) and then compute e8αe^{8\alpha}e8α.


  1. Rewrite using xxx as a function of yyy

Divide the equation by dydydy:

sec⁡2xdxdy+e2ytan⁡2x+tan⁡x=0\sec^2 x\frac{dx}{dy}+e^{2y}\tan^2 x+\tan x=0sec2xdydx​+e2ytan2x+tanx=0

Let

t=tan⁡xt=\tan xt=tanx

Then

dtdy=sec⁡2xdxdy\frac{dt}{dy}=\sec^2 x\frac{dx}{dy}dydt​=sec2xdydx​

So the differential equation becomes

dtdy+e2yt2+t=0\frac{dt}{dy}+e^{2y}t^2+t=0dydt​+e2yt2+t=0

That is,

dtdy+t=−e2yt2\frac{dt}{dy}+t=-e^{2y}t^2dydt​+t=−e2yt2

This is a Bernoulli-type equation.


  1. Use substitution u=1tu=\dfrac{1}{t}u=t1​

Let

u=1tu=\frac{1}{t}u=t1​

Then

dνdy=−1t2dtdy\frac{d\nu}{dy}=-\frac{1}{t^2}\frac{dt}{dy}dydν​=−t21​dydt​

From

dtdy+t=−e2yt2\frac{dt}{dy}+t=-e^{2y}t^2dydt​+t=−e2yt2

we get

dtdy=−t−e2yt2\frac{dt}{dy}=-t-e^{2y}t^2dydt​=−t−e2yt2

Hence

dνdy=−1t2(−t−e2yt2)=1t+e2y=ν+e2y\frac{d\nu}{dy}=-\frac{1}{t^2}(-t-e^{2y}t^2)=\frac{1}{t}+e^{2y}=\nu+e^{2y}dydν​=−t21​(−t−e2yt2)=t1​+e2y=ν+e2y

So

dνdy−ν=e2y\frac{d\nu}{dy}-\nu=e^{2y}dydν​−ν=e2y
  1. Solve the linear differential equation

The integrating factor is

IF=e−yIF=e^{-y}IF=e−y

Thus,

e−ydνdy−e−yν=eye^{-y}\frac{d\nu}{dy}-e^{-y}\nu=e^ye−ydydν​−e−yν=ey

which gives

ddy(νe−y)=ey\frac{d}{dy}(\nu e^{-y})=e^ydyd​(νe−y)=ey

Integrating,

νe−y=ey+C\nu e^{-y}=e^y+Cνe−y=ey+C

Therefore,

ν=e2y+Cey\nu=e^{2y}+Ce^yν=e2y+Cey

Since ν=1t=1tan⁡x=cot⁡x\nu=\dfrac{1}{t}=\dfrac{1}{\tan x}=\cot xν=t1​=tanx1​=cotx, we have

cot⁡x=e2y+Cey\cot x=e^{2y}+Ce^ycotx=e2y+Cey
  1. Use the initial condition

Given

y(π4)=0y\left(\frac{\pi}{4}\right)=0y(4π​)=0

At x=π4x=\frac{\pi}{4}x=4π​,

cot⁡π4=1\cot\frac{\pi}{4}=1cot4π​=1

and at y=0y=0y=0,

e2y=1,ey=1e^{2y}=1, \qquad e^y=1e2y=1,ey=1

So

1=1+C1=1+C1=1+C

which gives

C=0C=0C=0

Hence the relation simplifies to

cot⁡x=e2y\cot x=e^{2y}cotx=e2y
  1. Find α=y(π6)\alpha=y\left(\frac{\pi}{6}\right)α=y(6π​)

At

x=π6x=\frac{\pi}{6}x=6π​

we have

cot⁡π6=3\cot\frac{\pi}{6}=\sqrt{3}cot6π​=3​

So

e2α=3e^{2\alpha}=\sqrt{3}e2α=3​

Now square both sides:

e4α=3e^{4\alpha}=3e4α=3

Again square:

e8α=9e^{8\alpha}=9e8α=9
  1. Final answer
9\boxed{9}9​

The derived answer matches the stored correct answer.

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