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Differential Equations question

2022 · 27 Jul · Shift 1 · Q42
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  5. /2022 · 27 Jul · Shift 1 · Q42

Differential Equations question

2022 · 27 Jul · Shift 1 · Q42

JEE MainMathematicsDifferential EquationsNumerical+4 / −1
Let y=y(x)y=y(x)y=y(x) be the solution curve of the differential equation sin⁡(2x2)log⁡e(tan⁡x2)dy+(4xy−42xsin⁡(x2−π4))dx=0\sin \left( {2{x^2}} \right){\log _e}\left( {\tan {x^2}} \right)dy + \left( {4xy - 4\sqrt 2 x\sin \left( {{x^2} - {\pi \over 4}} \right)} \right)dx = 0sin(2x2)loge​(tanx2)dy+(4xy−42​xsin(x2−4π​))dx=0, 0<x<π20 \lt x \lt \sqrt {{\pi \over 2}}0<x<2π​​, which passes through the point (π6,1)\left(\sqrt{\frac{\pi}{6}}, 1\right)(6π​​,1). Then ∣y(π3)∣\left|y\left(\sqrt{\frac{\pi}{3}}\right)\right|​y(3π​​)​ is equal to ‾\underline{\hspace{2cm}}​.
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Correct answer: 1

  1. Write the differential equation in standard linear form

Given

sin⁡(2x2) ln⁡(tan⁡x2) dy+(4xy−42 xsin⁡(x2−π4))dx=0.\sin(2x^2)\,\ln(\tan x^2)\,dy + \left(4xy - 4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)\right)dx=0.sin(2x2)ln(tanx2)dy+(4xy−42​xsin(x2−4π​))dx=0.

Rewrite as

sin⁡(2x2)ln⁡(tan⁡x2)dydx+4xy−42 xsin⁡(x2−π4)=0.\sin(2x^2)\ln(\tan x^2)\frac{dy}{dx} + 4xy - 4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)=0.sin(2x2)ln(tanx2)dxdy​+4xy−42​xsin(x2−4π​)=0.

So,

sin⁡(2x2)ln⁡(tan⁡x2)dydx=42 xsin⁡(x2−π4)−4xy.\sin(2x^2)\ln(\tan x^2)\frac{dy}{dx}=4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)-4xy.sin(2x2)ln(tanx2)dxdy​=42​xsin(x2−4π​)−4xy.

Now use

sin⁡(2x2)=2sin⁡(x2)cos⁡(x2),\sin(2x^2)=2\sin(x^2)\cos(x^2),sin(2x2)=2sin(x2)cos(x2),

and

2sin⁡(x2−π4)=sin⁡x2−cos⁡x2.\sqrt2\sin\left(x^2-\frac\pi4\right)=\sin x^2-\cos x^2.2​sin(x2−4π​)=sinx2−cosx2.

Hence,

42 xsin⁡(x2−π4)=4x(sin⁡x2−cos⁡x2).4\sqrt2\,x\sin\left(x^2-\frac\pi4\right)=4x(\sin x^2-\cos x^2).42​xsin(x2−4π​)=4x(sinx2−cosx2).

Also,

sin⁡(2x2)=2sin⁡x2cos⁡x2.\sin(2x^2)=2\sin x^2\cos x^2.sin(2x2)=2sinx2cosx2.

Therefore,

\frac{dy}{dx}+ rac{4x}{\sin(2x^2)\ln(\tan x^2)}y =\frac{4x(\sin x^2-\cos x^2)}{2\sin x^2\cos x^2\ln(\tan x^2)}.

That is,

dydx+2xsin⁡x2cos⁡x2ln⁡(tan⁡x2)y=2x(sin⁡x2−cos⁡x2)sin⁡x2cos⁡x2ln⁡(tan⁡x2).\frac{dy}{dx}+\frac{2x}{\sin x^2\cos x^2\ln(\tan x^2)}y =\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2\ln(\tan x^2)}.dxdy​+sinx2cosx2ln(tanx2)2x​y=sinx2cosx2ln(tanx2)2x(sinx2−cosx2)​.
  1. Recognize useful derivatives

Since

tan⁡(x2)′=2xsec⁡2(x2),\tan(x^2)'=2x\sec^2(x^2),tan(x2)′=2xsec2(x2),

we get

ddxln⁡(tan⁡x2)=1tan⁡x2⋅2xsec⁡2(x2)=2xsin⁡x2cos⁡x2.\frac{d}{dx}\ln(\tan x^2)=\frac{1}{\tan x^2}\cdot 2x\sec^2(x^2) =\frac{2x}{\sin x^2\cos x^2}.dxd​ln(tanx2)=tanx21​⋅2xsec2(x2)=sinx2cosx22x​.

Thus the equation becomes

dydx+(ln⁡(tan⁡x2))′ln⁡(tan⁡x2)y=(ln⁡(tan⁡x2))′ln⁡(tan⁡x2)(sin⁡x2−cos⁡x2).\frac{dy}{dx}+\frac{\big(\ln(\tan x^2)\big)'}{\ln(\tan x^2)}y =\frac{\big(\ln(\tan x^2)\big)'}{\ln(\tan x^2)}(\sin x^2-\cos x^2).dxdy​+ln(tanx2)(ln(tanx2))′​y=ln(tanx2)(ln(tanx2))′​(sinx2−cosx2).

So it is a linear equation with integrating factor

I.F.=e∫(ln⁡(tan⁡x2))′ln⁡(tan⁡x2)dx=eln⁡∣ln⁡(tan⁡x2)∣=∣ln⁡(tan⁡x2)∣.\text{I.F.}=e^{\int \frac{(\ln(\tan x^2))'}{\ln(\tan x^2)}dx} = e^{\ln|\ln(\tan x^2)|} =|\ln(\tan x^2)|.I.F.=e∫ln(tanx2)(ln(tanx2))′​dx=eln∣ln(tanx2)∣=∣ln(tanx2)∣.

On the given interval and around the points used, we may take the integrating factor as

ln⁡(tan⁡x2).\ln(\tan x^2).ln(tanx2).
  1. Multiply throughout by the integrating factor

Then

ddx(yln⁡(tan⁡x2))=ddxln⁡(tan⁡x2)⋅(sin⁡x2−cos⁡x2).\frac{d}{dx}\left(y\ln(\tan x^2)\right) =\frac{d}{dx}\ln(\tan x^2)\cdot (\sin x^2-\cos x^2).dxd​(yln(tanx2))=dxd​ln(tanx2)⋅(sinx2−cosx2).

But notice

ddx(sin⁡x2−cos⁡x2)=2x(cos⁡x2+sin⁡x2),\frac{d}{dx}(\sin x^2-\cos x^2)=2x(\cos x^2+\sin x^2),dxd​(sinx2−cosx2)=2x(cosx2+sinx2),

so a better route is to check for a simpler exact derivative.

Observe from the original rearranged equation:

ln⁡(tan⁡x2)dydx+ddxln⁡(tan⁡x2) y=ddxln⁡(tan⁡x2) (sin⁡x2−cos⁡x2).\ln(\tan x^2)\frac{dy}{dx}+\frac{d}{dx}\ln(\tan x^2)\,y =\frac{d}{dx}\ln(\tan x^2)\,(\sin x^2-\cos x^2).ln(tanx2)dxdy​+dxd​ln(tanx2)y=dxd​ln(tanx2)(sinx2−cosx2).

Hence

ddx(yln⁡(tan⁡x2))=ddxln⁡(tan⁡x2) (sin⁡x2−cos⁡x2).\frac{d}{dx}\left(y\ln(\tan x^2)\right) =\frac{d}{dx}\ln(\tan x^2)\,(\sin x^2-\cos x^2).dxd​(yln(tanx2))=dxd​ln(tanx2)(sinx2−cosx2).

Now simplify the right-hand side:

ddxln⁡(tan⁡x2)=2xsin⁡x2cos⁡x2,\frac{d}{dx}\ln(\tan x^2)=\frac{2x}{\sin x^2\cos x^2},dxd​ln(tanx2)=sinx2cosx22x​,

so

ddxln⁡(tan⁡x2)(sin⁡x2−cos⁡x2)=2x(sin⁡x2−cos⁡x2)sin⁡x2cos⁡x2.\frac{d}{dx}\ln(\tan x^2)(\sin x^2-\cos x^2) =\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2}.dxd​ln(tanx2)(sinx2−cosx2)=sinx2cosx22x(sinx2−cosx2)​.

But

sin⁡x2−cos⁡x2sin⁡x2cos⁡x2=1cos⁡x2−1sin⁡x2=sec⁡x2−csc⁡x2.\frac{\sin x^2-\cos x^2}{\sin x^2\cos x^2} =\frac{1}{\cos x^2}-\frac{1}{\sin x^2} =\sec x^2-\csc x^2.sinx2cosx2sinx2−cosx2​=cosx21​−sinx21​=secx2−cscx2.

This suggests direct integration is cumbersome. Instead, try the substitution

z=y−(sin⁡x2+cos⁡x2).z=y-(\sin x^2+\cos x^2).z=y−(sinx2+cosx2).

Then

z′=y′−2xsin⁡x2+2xcos⁡x2=y′+2x(cos⁡x2−sin⁡x2).z'=y'-2x\sin x^2+2x\cos x^2 = y'+2x(\cos x^2-\sin x^2).z′=y′−2xsinx2+2xcosx2=y′+2x(cosx2−sinx2).

From the differential equation in linear form,

y′+2xsin⁡x2cos⁡x2ln⁡(tan⁡x2)y=2x(sin⁡x2−cos⁡x2)sin⁡x2cos⁡x2ln⁡(tan⁡x2).y'+\frac{2x}{\sin x^2\cos x^2\ln(\tan x^2)}y =\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2\ln(\tan x^2)}.y′+sinx2cosx2ln(tanx2)2x​y=sinx2cosx2ln(tanx2)2x(sinx2−cosx2)​.

Now note that

sin⁡x2cos⁡x2(sec⁡x2−csc⁡x2)=sin⁡x2−cos⁡x2.\sin x^2\cos x^2(\sec x^2-\csc x^2)=\sin x^2-\cos x^2.sinx2cosx2(secx2−cscx2)=sinx2−cosx2.

So the RHS is exactly

(ln⁡(tan⁡x2))′ln⁡(tan⁡x2)(sin⁡x2−cos⁡x2).\frac{(\ln(\tan x^2))'}{\ln(\tan x^2)}(\sin x^2-\cos x^2).ln(tanx2)(ln(tanx2))′​(sinx2−cosx2).

A natural trial solution is

y=sin⁡x2−cos⁡x2.y=\sin x^2-\cos x^2.y=sinx2−cosx2.

Check it:

y′=2xcos⁡x2+2xsin⁡x2=2x(sin⁡x2+cos⁡x2).y'=2x\cos x^2+2x\sin x^2=2x(\sin x^2+\cos x^2).y′=2xcosx2+2xsinx2=2x(sinx2+cosx2).

Then

y′+2xsin⁡x2cos⁡x2ln⁡(tan⁡x2)y=2x(sin⁡x2+cos⁡x2)+2x(sin⁡x2−cos⁡x2)sin⁡x2cos⁡x2ln⁡(tan⁡x2),y'+\frac{2x}{\sin x^2\cos x^2\ln(\tan x^2)}y =2x(\sin x^2+\cos x^2)+\frac{2x(\sin x^2-\cos x^2)}{\sin x^2\cos x^2\ln(\tan x^2)},y′+sinx2cosx2ln(tanx2)2x​y=2x(sinx2+cosx2)+sinx2cosx2ln(tanx2)2x(sinx2−cosx2)​,

which does not match. So instead solve systematically.

  1. Use the substitution t=ln⁡(tan⁡x2)t=\ln(\tan x^2)t=ln(tanx2)

Then

dtdx=2xsin⁡x2cos⁡x2.\frac{dt}{dx}=\frac{2x}{\sin x^2\cos x^2}.dxdt​=sinx2cosx22x​.

The differential equation becomes

dydx+t′ty=t′t(sin⁡x2−cos⁡x2).\frac{dy}{dx}+\frac{t'}{t}y=\frac{t'}{t}(\sin x^2-\cos x^2).dxdy​+tt′​y=tt′​(sinx2−cosx2).

Multiply by ttt:

tdydx+t′y=t′(sin⁡x2−cos⁡x2).t\frac{dy}{dx}+t'y=t'(\sin x^2-\cos x^2).tdxdy​+t′y=t′(sinx2−cosx2).

Thus

ddx(ty)=t′(sin⁡x2−cos⁡x2).\frac{d}{dx}(ty)=t'(\sin x^2-\cos x^2).dxd​(ty)=t′(sinx2−cosx2).

Now let u=x2u=x^2u=x2. Then du=2x dxdu=2x\,dxdu=2xdx, and

t=ln⁡(tan⁡u),t′ dx=d(ln⁡(tan⁡u)).t=\ln(\tan u), \qquad t'\,dx=d(\ln(\tan u)).t=ln(tanu),t′dx=d(ln(tanu)).

So

ty=∫(sin⁡u−cos⁡u) d(ln⁡(tan⁡u))+C.ty=\int (\sin u-\cos u)\,d(\ln(\tan u))+C.ty=∫(sinu−cosu)d(ln(tanu))+C.

Use

d(ln⁡(tan⁡u))=dusin⁡ucos⁡u.d(\ln(\tan u))=\frac{du}{\sin u\cos u}.d(ln(tanu))=sinucosudu​.

Hence

∫(sin⁡u−cos⁡u) d(ln⁡(tan⁡u))=∫sin⁡u−cos⁡usin⁡ucos⁡u du=∫(sec⁡u−csc⁡u) du.\int (\sin u-\cos u)\,d(\ln(\tan u)) =\int \frac{\sin u-\cos u}{\sin u\cos u}\,du =\int (\sec u-\csc u)\,du.∫(sinu−cosu)d(ln(tanu))=∫sinucosusinu−cosu​du=∫(secu−cscu)du.

Now,

∫sec⁡u du=ln⁡∣sec⁡u+tan⁡u∣,\int \sec u\,du=\ln|\sec u+\tan u|,∫secudu=ln∣secu+tanu∣, ∫csc⁡u du=ln⁡∣csc⁡u−cot⁡u∣.\int \csc u\,du=\ln|\csc u-\cot u|.∫cscudu=ln∣cscu−cotu∣.

Therefore,

∫(sec⁡u−csc⁡u)du=ln⁡∣sec⁡u+tan⁡u∣−ln⁡∣csc⁡u−cot⁡u∣+C.\int (\sec u-\csc u)du =\ln|\sec u+\tan u| - \ln|\csc u-\cot u| + C.∫(secu−cscu)du=ln∣secu+tanu∣−ln∣cscu−cotu∣+C.

Using identities,

sec⁡u+tan⁡u=1+sin⁡ucos⁡u,csc⁡u−cot⁡u=1−cos⁡usin⁡u.\sec u+\tan u=\frac{1+\sin u}{\cos u}, \qquad \csc u-\cot u=\frac{1-\cos u}{\sin u}.secu+tanu=cosu1+sinu​,cscu−cotu=sinu1−cosu​.

This simplifies, but we do not actually need the full closed form. We use the given points where u=π6u=\frac\pi6u=6π​ and u=π3u=\frac\pi3u=3π​.

  1. Apply the initial condition

At

x=π6,u=π6,x=\sqrt{\frac\pi6}, \quad u=\frac\pi6,x=6π​​,u=6π​,

we have

y=1,y=1,y=1,

and

t=ln⁡(tan⁡π6)=ln⁡(13)=−12ln⁡3.t=\ln\left(\tan\frac\pi6\right)=\ln\left(\frac1{\sqrt3}\right)=-\frac12\ln 3.t=ln(tan6π​)=ln(3​1​)=−21​ln3.

So

ty=−12ln⁡3.ty=-\frac12\ln 3.ty=−21​ln3.

Now evaluate the integral from u=π6u=\frac\pi6u=6π​ to u=π3u=\frac\pi3u=3π​:

(ty)∣π/3−(ty)∣π/6=∫π/6π/3(sec⁡u−csc⁡u)du.(ty)\Big|_{\pi/3}-(ty)\Big|_{\pi/6} =\int_{\pi/6}^{\pi/3}(\sec u-\csc u)du.(ty)​π/3​−(ty)​π/6​=∫π/6π/3​(secu−cscu)du.

But note the symmetry:

sec⁡(π2−u)=csc⁡u,csc⁡(π2−u)=sec⁡u.\sec\left(\frac\pi2-u\right)=\csc u, \qquad \csc\left(\frac\pi2-u\right)=\sec u.sec(2π​−u)=cscu,csc(2π​−u)=secu.

Since the interval [π6,π3]\left[\frac\pi6,\frac\pi3\right][6π​,3π​] is symmetric about π4\frac\pi44π​, we get

∫π/6π/3sec⁡u du=∫π/6π/3csc⁡u du.\int_{\pi/6}^{\pi/3}\sec u\,du = \int_{\pi/6}^{\pi/3}\csc u\,du.∫π/6π/3​secudu=∫π/6π/3​cscudu.

Hence

∫π/6π/3(sec⁡u−csc⁡u)du=0.\int_{\pi/6}^{\pi/3}(\sec u-\csc u)du=0.∫π/6π/3​(secu−cscu)du=0.

Therefore,

(ty)∣π/3=(ty)∣π/6=−12ln⁡3.(ty)\Big|_{\pi/3}=(ty)\Big|_{\pi/6}=-\frac12\ln 3.(ty)​π/3​=(ty)​π/6​=−21​ln3.

At x=π3x=\sqrt{\frac\pi3}x=3π​​, i.e. u=π3u=\frac\pi3u=3π​,

t=ln⁡(tan⁡π3)=ln⁡(3)=12ln⁡3.t=\ln\left(\tan\frac\pi3\right)=\ln(\sqrt3)=\frac12\ln 3.t=ln(tan3π​)=ln(3​)=21​ln3.

Thus

12ln⁡3⋅y(π3)=−12ln⁡3.\frac12\ln 3\cdot y\left(\sqrt{\frac\pi3}\right)=-\frac12\ln 3.21​ln3⋅y(3π​​)=−21​ln3.

So

y(π3)=−1.y\left(\sqrt{\frac\pi3}\right)=-1.y(3π​​)=−1.

Hence

∣y(π3)∣=1.\left|y\left(\sqrt{\frac\pi3}\right)\right|=1.​y(3π​​)​=1.
  1. Final answer
1\boxed{1}1​
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