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Differential Equations question

2021 · 18 Mar · Shift 2 · Q40
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  5. /2021 · 18 Mar · Shift 2 · Q40

Differential Equations question

2021 · 18 Mar · Shift 2 · Q40

JEE MainMathematicsDifferential EquationsNumerical+4 / −1
Let y = y(x) be the solution of the differential equation xdy −-− ydx =(x2−y2)dx\sqrt {({x^2} - {y^2})} dx(x2−y2)​dx, x ≥\ge≥ 1, with y(1) = 0. If the area bounded by the line x = 1, x = e π\piπ, y = 0 and y = y(x) is α\alphaα e2 π\piπ+β\betaβ, then the value of 10(α\alphaα+β\betaβ) is equal to ‾\underline{\hspace{2cm}}​.
Numerical answer
View written solutionFree

Correct answer: 4

  1. Rewrite the differential equation

Given x dy−y dx=x2−y2 dx,x≥1,y(1)=0.x\,dy - y\,dx = \sqrt{x^2-y^2}\,dx, \qquad x\ge 1, \qquad y(1)=0.xdy−ydx=x2−y2​dx,x≥1,y(1)=0.

Divide by dxdxdx: xdydx−y=x2−y2.x\frac{dy}{dx}-y=\sqrt{x^2-y^2}.xdxdy​−y=x2−y2​.

So, x y′−y=x2−y2.x\,y' - y = \sqrt{x^2-y^2}.xy′−y=x2−y2​.


  1. Use the substitution y=vxy=vxy=vx

Let y=vx⇒y′=v+xdvdx.y=vx \quad \Rightarrow \quad y'=v+x\frac{dv}{dx}.y=vx⇒y′=v+xdxdv​.

Substitute into the equation: x(v+xdvdx)−vx=x2−v2x2.x\left(v+x\frac{dv}{dx}\right)-vx=\sqrt{x^2-v^2x^2}.x(v+xdxdv​)−vx=x2−v2x2​.

The xvxvxv terms cancel: x2dvdx=x1−v2.x^2\frac{dv}{dx}=x\sqrt{1-v^2}.x2dxdv​=x1−v2​.

Since x≥1>0x\ge 1>0x≥1>0, xdvdx=1−v2.x\frac{dv}{dx}=\sqrt{1-v^2}.xdxdv​=1−v2​.

Separate variables: dv1−v2=dxx.\frac{dv}{\sqrt{1-v^2}}=\frac{dx}{x}.1−v2​dv​=xdx​.

Integrate: sin⁡−1v=ln⁡x+C.\sin^{-1}v=\ln x + C.sin−1v=lnx+C.

Using y(1)=0y(1)=0y(1)=0, we get v(1)=0v(1)=0v(1)=0, so sin⁡−1(0)=ln⁡1+C⇒0=0+C⇒C=0.\sin^{-1}(0)=\ln 1 + C \Rightarrow 0=0+C \Rightarrow C=0.sin−1(0)=ln1+C⇒0=0+C⇒C=0.

Hence sin⁡−1v=ln⁡x⇒v=sin⁡(ln⁡x).\sin^{-1}v=\ln x \quad \Rightarrow \quad v=\sin(\ln x).sin−1v=lnx⇒v=sin(lnx).

Therefore, y=xsin⁡(ln⁡x).\boxed{y=x\sin(\ln x)}.y=xsin(lnx)​.


  1. Set up the required area

The area bounded by x=1x=1x=1, x=eπx=e^{\pi}x=eπ, y=0y=0y=0, and y=y(x)y=y(x)y=y(x) is A=∫1eπy dx=∫1eπxsin⁡(ln⁡x) dx.A=\int_1^{e^\pi} y\,dx = \int_1^{e^\pi} x\sin(\ln x)\,dx.A=∫1eπ​ydx=∫1eπ​xsin(lnx)dx.


  1. Evaluate the integral

Let t=ln⁡x⇒x=et,dx=etdt.t=\ln x \Rightarrow x=e^t, \quad dx=e^t dt.t=lnx⇒x=et,dx=etdt.

Then xsin⁡(ln⁡x) dx=etsin⁡t⋅etdt=e2tsin⁡t dt.x\sin(\ln x)\,dx = e^t\sin t \cdot e^t dt = e^{2t}\sin t\,dt.xsin(lnx)dx=etsint⋅etdt=e2tsintdt.

When x=1x=1x=1, t=0t=0t=0; when x=eπx=e^\pix=eπ, t=πt=\pit=π.

So, A=∫0πe2tsin⁡t dt.A=\int_0^\pi e^{2t}\sin t\,dt.A=∫0π​e2tsintdt.

Use the standard result ∫eatsin⁡bt dt=eata2+b2(asin⁡bt−bcos⁡bt).\int e^{at}\sin bt\,dt = \frac{e^{at}}{a^2+b^2}(a\sin bt - b\cos bt).∫eatsinbtdt=a2+b2eat​(asinbt−bcosbt).

Here a=2a=2a=2, b=1b=1b=1, so ∫e2tsin⁡t dt=e2t5(2sin⁡t−cos⁡t).\int e^{2t}\sin t\,dt = \frac{e^{2t}}{5}(2\sin t - \cos t).∫e2tsintdt=5e2t​(2sint−cost).

Thus A=[e2t5(2sin⁡t−cos⁡t)]0π.A=\left[\frac{e^{2t}}{5}(2\sin t - \cos t)\right]_0^\pi.A=[5e2t​(2sint−cost)]0π​.

Now evaluate:

  • At t=πt=\pit=π: sin⁡π=0\sin\pi=0sinπ=0, cos⁡π=−1\cos\pi=-1cosπ=−1 e2π5(0−(−1))=e2π5.\frac{e^{2\pi}}{5}(0-(-1))=\frac{e^{2\pi}}{5}.5e2π​(0−(−1))=5e2π​.
  • At t=0t=0t=0: sin⁡0=0\sin0=0sin0=0, cos⁡0=1\cos0=1cos0=1 15(0−1)=−15.\frac{1}{5}(0-1)=-\frac{1}{5}.51​(0−1)=−51​.

Hence A=e2π5−(−15)=e2π5+15.A=\frac{e^{2\pi}}{5}-\left(-\frac{1}{5}\right)=\frac{e^{2\pi}}{5}+\frac{1}{5}.A=5e2π​−(−51​)=5e2π​+51​.

So in the form A=αe2π+β,A=\alpha e^{2\pi}+\beta,A=αe2π+β, we have α=15,β=15.\alpha=\frac15, \qquad \beta=\frac15.α=51​,β=51​.

Therefore, 10(α+β)=10(15+15)=10⋅25=4.10(\alpha+\beta)=10\left(\frac15+\frac15\right)=10\cdot \frac25=4.10(α+β)=10(51​+51​)=10⋅52​=4.


  1. Comparison with stored answer

Derived answer: 4\boxed{4}4​.

Stored correct answer: 444.

They agree.

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