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Differential Equations question

2024 · 31 Jan · Shift 1 · Q37
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  5. /2024 · 31 Jan · Shift 1 · Q37

Differential Equations question

2024 · 31 Jan · Shift 1 · Q37

JEE MainMathematicsDifferential EquationsMCQ+4 / −1
Let y=y(x)y=y(x)y=y(x) be the solution of the differential equation dydx=(tan⁡x)+ysin⁡x(sec⁡x−sin⁡xtan⁡x),x∈(0,π2)\frac{d y}{d x}=\frac{(\tan x)+y}{\sin x(\sec x-\sin x \tan x)}, x \in\left(0, \frac{\pi}{2}\right)dxdy​=sinx(secx−sinxtanx)(tanx)+y​,x∈(0,2π​) satisfying the condition y(π4)=2y\left(\frac{\pi}{4}\right)=2y(4π​)=2. Then, y(π3)y\left(\frac{\pi}{3}\right)y(3π​) is
  1. A
    3(2+log⁡e3)\sqrt{3}\left(2+\log _e 3\right)3​(2+loge​3)
  2. B
    3(1+2log⁡e3)\sqrt{3}\left(1+2 \log _e 3\right)3​(1+2loge​3)
  3. C
    3(2+log⁡e3)\sqrt{3}\left(2+\log _e \sqrt{3}\right)3​(2+loge​3​)
  4. D
    32(2+log⁡e3)\frac{\sqrt{3}}{2}\left(2+\log _e 3\right)23​​(2+loge​3)
View written solutionFree

Correct answer: C

  1. Simplify the differential equation

Given

dydx=tan⁡x+ysin⁡x(sec⁡x−sin⁡xtan⁡x),x∈(0,π2)\frac{dy}{dx}=\frac{\tan x+y}{\sin x(\sec x-\sin x\tan x)}, \qquad x\in\left(0,\frac\pi2\right)dxdy​=sinx(secx−sinxtanx)tanx+y​,x∈(0,2π​)

First simplify the denominator:

sec⁡x−sin⁡xtan⁡x=1cos⁡x−sin⁡x⋅sin⁡xcos⁡x=1−sin⁡2xcos⁡x=cos⁡2xcos⁡x=cos⁡x\sec x-\sin x\tan x=\frac1{\cos x}-\sin x\cdot\frac{\sin x}{\cos x} =\frac{1-\sin^2 x}{\cos x}=\frac{\cos^2 x}{\cos x}=\cos xsecx−sinxtanx=cosx1​−sinx⋅cosxsinx​=cosx1−sin2x​=cosxcos2x​=cosx

So,

sin⁡x(sec⁡x−sin⁡xtan⁡x)=sin⁡xcos⁡x\sin x(\sec x-\sin x\tan x)=\sin x\cos xsinx(secx−sinxtanx)=sinxcosx

Hence the DE becomes

dydx=tan⁡x+ysin⁡xcos⁡x\frac{dy}{dx}=\frac{\tan x+y}{\sin x\cos x}dxdy​=sinxcosxtanx+y​

Now,

tan⁡xsin⁡xcos⁡x=sin⁡x/cos⁡xsin⁡xcos⁡x=1cos⁡2x=sec⁡2x\frac{\tan x}{\sin x\cos x}=\frac{\sin x/\cos x}{\sin x\cos x}=\frac1{\cos^2 x}=\sec^2 xsinxcosxtanx​=sinxcosxsinx/cosx​=cos2x1​=sec2x

Therefore,

dydx=sec⁡2x+ysin⁡xcos⁡x\frac{dy}{dx}=\sec^2 x+\frac{y}{\sin x\cos x}dxdy​=sec2x+sinxcosxy​

or

dydx−1sin⁡xcos⁡xy=sec⁡2x\frac{dy}{dx}-\frac{1}{\sin x\cos x}y=\sec^2 xdxdy​−sinxcosx1​y=sec2x

This is a linear differential equation.


  1. Write in standard linear form
dydx+P(x)y=Q(x)\frac{dy}{dx}+P(x)y=Q(x)dxdy​+P(x)y=Q(x)

with

P(x)=−1sin⁡xcos⁡x,Q(x)=sec⁡2xP(x)=-\frac{1}{\sin x\cos x}, \qquad Q(x)=\sec^2 xP(x)=−sinxcosx1​,Q(x)=sec2x

The integrating factor is

I.F.=e∫P(x) dx=e−∫dxsin⁡xcos⁡x\text{I.F.}=e^{\int P(x)\,dx}=e^{-\int \frac{dx}{\sin x\cos x}}I.F.=e∫P(x)dx=e−∫sinxcosxdx​

Now,

1sin⁡xcos⁡x=tan⁡x+cot⁡x\frac{1}{\sin x\cos x}=\tan x+\cot xsinxcosx1​=tanx+cotx

So,

∫dxsin⁡xcos⁡x=∫(tan⁡x+cot⁡x) dx\int \frac{dx}{\sin x\cos x}=\int (\tan x+\cot x)\,dx∫sinxcosxdx​=∫(tanx+cotx)dx =∫tan⁡x dx+∫cot⁡x dx=\int \tan x\,dx+\int \cot x\,dx=∫tanxdx+∫cotxdx =−ln⁡(cos⁡x)+ln⁡(sin⁡x)=ln⁡(tan⁡x)=-\ln(\cos x)+\ln(\sin x)=\ln(\tan x)=−ln(cosx)+ln(sinx)=ln(tanx)

Thus,

I.F.=e−ln⁡(tan⁡x)=1tan⁡x=cot⁡x\text{I.F.}=e^{-\ln(\tan x)}=\frac{1}{\tan x}=\cot xI.F.=e−ln(tanx)=tanx1​=cotx
  1. Multiply the DE by the integrating factor

Multiplying by cot⁡x\cot xcotx:

cot⁡xdydx−cot⁡x⋅1sin⁡xcos⁡xy=cot⁡xsec⁡2x\cot x\frac{dy}{dx}-\cot x\cdot\frac{1}{\sin x\cos x}y=\cot x\sec^2 xcotxdxdy​−cotx⋅sinxcosx1​y=cotxsec2x

The left side becomes

ddx(ycot⁡x)\frac{d}{dx}(y\cot x)dxd​(ycotx)

And the right side simplifies as

cot⁡xsec⁡2x=cos⁡xsin⁡x⋅1cos⁡2x=1sin⁡xcos⁡x\cot x\sec^2 x=\frac{\cos x}{\sin x}\cdot\frac{1}{\cos^2 x}=\frac{1}{\sin x\cos x}cotxsec2x=sinxcosx​⋅cos2x1​=sinxcosx1​

So,

ddx(ycot⁡x)=1sin⁡xcos⁡x\frac{d}{dx}(y\cot x)=\frac{1}{\sin x\cos x}dxd​(ycotx)=sinxcosx1​

Integrating,

ycot⁡x=∫dxsin⁡xcos⁡x+C=ln⁡(tan⁡x)+Cy\cot x=\int \frac{dx}{\sin x\cos x}+C=\ln(\tan x)+Cycotx=∫sinxcosxdx​+C=ln(tanx)+C

Hence,

y=tan⁡x [ln⁡(tan⁡x)+C]y=\tan x\,[\ln(\tan x)+C]y=tanx[ln(tanx)+C]
  1. Use the initial condition

Given

y(π4)=2y\left(\frac\pi4\right)=2y(4π​)=2

Since

tan⁡π4=1,ln⁡1=0\tan\frac\pi4=1, \qquad \ln 1=0tan4π​=1,ln1=0

we get

2=1⋅(0+C)2=1\cdot(0+C)2=1⋅(0+C)

so

C=2C=2C=2

Therefore the solution is

y=tan⁡x (ln⁡(tan⁡x)+2)y=\tan x\,(\ln(\tan x)+2)y=tanx(ln(tanx)+2)
  1. Find y(π3)y\left(\frac\pi3\right)y(3π​)

Now,

tan⁡π3=3\tan\frac\pi3=\sqrt3tan3π​=3​

Thus,

y(π3)=3(ln⁡(3)+2)y\left(\frac\pi3\right)=\sqrt3\left(\ln(\sqrt3)+2\right)y(3π​)=3​(ln(3​)+2)

So,

y(π3)=3(2+ln⁡3)\boxed{y\left(\frac\pi3\right)=\sqrt3\left(2+\ln\sqrt3\right)}y(3π​)=3​(2+ln3​)​
  1. Evaluate the options
  • A: 3(2+ln⁡3)\sqrt3(2+\ln 3)3​(2+ln3) — not equal
  • B: 3(1+2ln⁡3)\sqrt3(1+2\ln 3)3​(1+2ln3) — not equal
  • C: 3(2+ln⁡3)\sqrt3(2+\ln\sqrt3)3​(2+ln3​) — correct
  • D: 32(2+ln⁡3)\dfrac{\sqrt3}{2}(2+\ln 3)23​​(2+ln3) — note that ln⁡3=12ln⁡3\ln\sqrt3=\frac12\ln 3ln3​=21​ln3, so 3(2+ln⁡3)=3(2+12ln⁡3)\sqrt3\left(2+\ln\sqrt3\right)=\sqrt3\left(2+\frac12\ln 3\right)3​(2+ln3​)=3​(2+21​ln3) which is not the same as option D.

Hence the correct option is C.

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