Differential Equations

JEE Mathematics · 179 questions · Page 7 of 18 · Click an option or "Show Solution" to reveal answer

Q61
Let y = y(x) be solution of the differential equation log(dydx)=3x+4y{\log _{}}\left( {{{dy} \over {dx}}} \right) = 3x + 4y, with y(0) = 0. If y(23loge2)=αloge2y\left( { - {2 \over 3}{{\log }_e}2} \right) = \alpha {\log _e}2, then the value of α\alpha is equal to :
A 14 - {1 \over 4}
B 14{1 \over 4}
C 22
D 12 - {1 \over 2}
Correct Answer
Option A
Solution
dydx=e3x.e4ye4ydy=e3xdx{{dy} \over {dx}} = {e^{3x}}.{e^{4y}} \Rightarrow \int {{e^{ - 4y}}dy = \int {{e^{3x}}dx} }
e4y4=e3x3+C1413=CC=712{{{e^{ - 4y}}} \over { - 4}} = {{{e^{3x}}} \over 3} + C \Rightarrow - {1 \over 4} - {1 \over 3} = C \Rightarrow C = - {7 \over {12}}
e4y4=e3x3712e4y=4e3x73{{{e^{ - 4y}}} \over { - 4}} = {{{e^{3x}}} \over 3} - {7 \over {12}} \Rightarrow {e^{ - 4y}} = {{4{e^{3x}} - 7} \over { - 3}}
e4y=374e3x4y=ln(374e3x){e^{4y}} = {3 \over {7 - 4{e^{3x}}}} \Rightarrow 4y = \ln \left( {{3 \over {7 - 4{e^{3x}}}}} \right)
4y=ln(36)4y = \ln \left( {{3 \over 6}} \right)

when

x=23ln2x = - {2 \over 3}\ln 2
y=14ln(12)=14ln2y = {1 \over 4}\ln \left( {{1 \over 2}} \right) = - {1 \over 4}\ln 2
Q62
Let y = y(x) be the solution of the differential equation dydx=(y+1)((y+1)ex2/2x){{dy} \over {dx}} = (y + 1)\left( {(y + 1){e^{{x^2}/2}} - x} \right), 0 < x < 2.1, with y(2) = 0. Then the value of dydx{{dy} \over {dx}} at x = 1 is equal to :
A e5/2(1+e2)2{{{e^{5/2}}} \over {{{(1 + {e^2})}^2}}}
B 5e1/2(e2+1)2{{5{e^{1/2}}} \over {{{({e^2} + 1)}^2}}}
C 2e2(1+e2)2 - {{2{e^2}} \over {{{(1 + {e^2})}^2}}}
D e3/2(e2+1)2{{ - {e^{3/2}}} \over {{{({e^2} + 1)}^2}}}
Correct Answer
Option D
Solution
dydx=(y+1)((y+1)ex22x){{dy} \over {dx}} = (y + 1)\left( {(y + 1){e^{{{{x^2}} \over 2}}} - x} \right)
1(y+1)2dydxx(1y+1)=ex22\Rightarrow {{ - 1} \over {{{(y + 1)}^2}}}{{dy} \over {dx}} - x\left( {{1 \over {y + 1}}} \right) = - {e^{{{{x^2}} \over 2}}}

Put,

1y+1=z{1 \over {y + 1}} = z
1(y+1)2.dydx=dzdx- {1 \over {{{(y + 1)}^2}}}.{{dy} \over {dx}} = {{dz} \over {dx}}

\therefore

dzdx+z(x)=ex22{{dz} \over {dx}} + z( - x) = - {e^{{{{x^2}} \over 2}}}
I.F=exdx=ex22I.F = {e^{\int { - xdx} }} = {e^{{{ - {x^2}} \over 2}}}
z.(ex22)=ex22.ex22dx=1.dx=x+Cz.\left( {{e^{ - {{{x^2}} \over 2}}}} \right) = - \int {{e^{ - {{{x^2}} \over 2}}}.{e^{{{{x^2}} \over 2}}}dx} = - \int {1.dx = - x + C}
ex22y+1=x+C\Rightarrow {{{e^{ - {{{x^2}} \over 2}}}} \over {y + 1}} = - x + C

.... (1) Given y = 0 at x = 2 Put in (1)

e20+1=2+C{{{e^{ - 2}}} \over {0 + 1}} = - 2 + C
C=e2+2C = {e^{ - 2}} + 2

.... (2) From (1) and (2)

y+1=ex22e2+2xy + 1 = {{{e^{ - {{{x^2}} \over 2}}}} \over {{e^{ - 2}} + 2 - x}}

Again, at x = 1

y+1=e3/2e2+1\Rightarrow y + 1 = {{{e^{3/2}}} \over {{e^2} + 1}}
y+1=e3/2e2+1\Rightarrow y + 1 = {{{e^{3/2}}} \over {{e^2} + 1}}

\therefore

dydxx=1=e3/2e2+1(e3/2e2+1×e1/21){\left. {{{dy} \over {dx}}} \right|_{x = 1}} = {{{e^{3/2}}} \over {{e^2} + 1}}\left( {{{{e^{3/2}}} \over {{e^2} + 1}} \times {e^{1/2}} - 1} \right)
=e3/2(e2+1)2= - {{{e^{3/2}}} \over {{{({e^2} + 1)}^2}}}
Q63
Let y = y(x) be the solution of the differential equation xtan(yx)dy=(ytan(yx)x)dxx\tan \left( {{y \over x}} \right)dy = \left( {y\tan \left( {{y \over x}} \right) - x} \right)dx, 1x1 - 1 \le x \le 1, y(12)=π6y\left( {{1 \over 2}} \right) = {\pi \over 6}. Then the area of the region bounded by the curves x = 0, x=12x = {1 \over {\sqrt 2 }} and y = y(x) in the upper half plane is :
A 18(π1){1 \over 8}(\pi - 1)
B 112(π3){1 \over {12}}(\pi - 3)
C 14(π2){1 \over 4}(\pi - 2)
D 16(π1){1 \over 6}(\pi - 1)
Correct Answer
Option A
Solution

We have,

dydx=x(yx.tanyx1)xtanyx{{dy} \over {dx}} = {{x\left( {{y \over x}.\tan {y \over x} - 1} \right)} \over {x\tan {y \over x}}}

\therefore

dydx=yxcot(yx){{dy} \over {dx}} = {y \over x} - \cot \left( {{y \over x}} \right)

Put

yx=v{y \over x} = v
y=vn\Rightarrow y = vn

\therefore

dydx=v+ndvdx{{dy} \over {dx}} = v + {{ndv} \over {dx}}

Now, we get

v+ndvdx=vcot(v)v + n{{dv} \over {dx}} = v - \cot (v)
(tan)dv=dxx\Rightarrow \int {(\tan )dv} = - \int {{{dx} \over x}}

\therefore

lnsec(yx)=lnx+c\ln \left| {\sec \left( {{y \over x}} \right)} \right| = - \ln \left| x \right| + c

As,

(12)=(yx)C=0\left( {{1 \over 2}} \right) = \left( {{y \over x}} \right) \Rightarrow C = 0

\therefore

sec(yx)=1x\sec \left( {{y \over x}} \right) = {1 \over x}
cos(yx)=x\Rightarrow \cos \left( {{y \over x}} \right) = x

\therefore

y=xcos1(x)y = x{\cos ^{ - 1}}(x)

So, required bounded area

=012x(II)(cos1x(I))dx=(π18)= \int\limits_0^{{1 \over {\sqrt 2 }}} {\mathop x\limits_{(II)} (\mathop {{{\cos }^{ - 1}}x}\limits_{(I)} )dx = \left( {{{\pi - 1} \over 8}} \right)}

(I. B. P.) \therefore Option (1) is correct.

Q64
Let y = y(x) be the solution of the differential equation ex1y2dx+(yx)dy=0{e^x}\sqrt {1 - {y^2}} dx + \left( {{y \over x}} \right)dy = 0, y(1) = -1. Then the value of (y(3))2 is equal to :
A 1 - 4e3
B 1 - 4e6
C 1 + 4e3
D 1 + 4e6
Correct Answer
Option B
Solution
ex1y2dx+yxdy=0{e^x}\sqrt {1 - {y^2}} dx + {y \over x}dy = 0
ex1y2dx+yxdy\Rightarrow {e^x}\sqrt {1 - {y^2}} dx + {{ - y} \over x}dy
y1y2dy=IIex1xdx\Rightarrow \int {{{ - y} \over {\sqrt {1 - {y^2}} }}} dy = \int_{II}^{{e^x}} {_1^xdx}
1y2=ex(x1)+c\Rightarrow \sqrt {1 - {y^2}} = {e^x}(x - 1) + c

Given : At x = 1, y = -1 \Rightarrow 0 = 0 + c \Rightarrow c = 0 \therefore

1y2=ex(x1)\sqrt {1 - {y^2}} = {e^x}(x - 1)

At x = 3

1y2=(e32)2y2=14e61 - {y^2} = {({e^3}2)^2} \Rightarrow {y^2} = 1 - 4{e^6}
Q65
Let y = y(x) satisfies the equation dydxA=0{{dy} \over {dx}} - |A| = 0, for all x > 0, where A=[ysinx1011201x]A = \left[ \begin{array}{lll}y & {\sin x} & 1 \\ 0 & { - 1} & 1 \\ 2 & 0 & {{1 \over x}} \end{array} \right]. If y(π)=π+2y(\pi ) = \pi + 2, then the value of y(π2)y\left( {{\pi \over 2}} \right) is :
A π2+4π{\pi \over 2} + {4 \over \pi }
B π21π{\pi \over 2} - {1 \over \pi }
C 3π21π{{3\pi } \over 2} - {1 \over \pi }
D π24π{\pi \over 2} - {4 \over \pi }
Correct Answer
Option A
Solution
A=yx+2sinx+2|A| = - {y \over x} + 2\sin x + 2
dydx=A{{dy} \over {dx}} = |A|
dydx=yx+2sinx+2{{dy} \over {dx}} = - {y \over x} + 2\sin x + 2
dydx+yx=2sinx+2{{dy} \over {dx}} + {y \over x} = 2\sin x + 2
I.F.=e1xdx=xI.F. = {e^{\int {{1 \over x}dx} }} = x
yx=x(2sinx+2)dx\Rightarrow yx = \int {x(2\sin x + 2)dx}
xy=x22xcosx+2sinx+cxy = {x^2} - 2x\cos x + 2\sin x + c

..... (i) Now, x = π\pi, y = π\pi + 2 Use in (i) c = 0 Now, (i) becomes

xy=x22xcosx+2sinxxy = {x^2} - 2x\cos x + 2\sin x

put

x=π/2x = \pi /2
π2y=(π2)22.π2cosπ2+2sinπ2{\pi \over 2}y = {\left( {{\pi \over 2}} \right)^2} - 2.{\pi \over 2}\cos {\pi \over 2} + 2\sin {\pi \over 2}
y(π2)=π24+2y({\pi \over 2}) = {{{\pi ^2}} \over 4} + 2
Q66
Let y = y(x) be the solution of the differential equation cosec2xdy+2dx=(1+ycos2x)cosec2xdx\cos e{c^2}xdy + 2dx = (1 + y\cos 2x)\cos e{c^2}xdx, with y(π4)=0y\left( {{\pi \over 4}} \right) = 0. Then, the value of (y(0)+1)2{(y(0) + 1)^2} is equal to :
A e1/2
B e-1/2
C e-1
D e
Correct Answer
Option C
Solution
dydx+2sin2x=1+ycos2x{{dy} \over {dx}} + 2{\sin ^2}x = 1 + y\cos 2x
dydx+(cos2x)y=cos2x\Rightarrow {{dy} \over {dx}} + ( - \cos 2x)y = \cos 2x
I.F.=ecos2xdx=esin2x2I.F. = {e^{\int { - \cos 2xdx} }} = {e^{ - {{\sin 2x} \over 2}}}

Solution of D.E.

y(esin2x2)=(cos2x)(esin2x2)dx+cy\left( {{e^{ - {{\sin 2x} \over 2}}}} \right) = \int {(\cos 2x)\left( {{e^{ - {{\sin 2x} \over 2}}}} \right)} dx + c
y(esin2x2)=esin2x2+c\Rightarrow y\left( {{e^{ - {{\sin 2x} \over 2}}}} \right) = - {e^{ - {{\sin 2x} \over 2}}} + c

Given

y(π4)=0y\left( {{\pi \over 4}} \right) = 0
0=e12+cc=e12\Rightarrow 0 = - {e^{{{ - 1} \over 2}}} + c \Rightarrow c = {e^{{{ - 1} \over 2}}}
y(esin2x2)=esin2x2+e12\Rightarrow y\left( {{e^{ - {{\sin 2x} \over 2}}}} \right) = - {e^{ - {{\sin 2x} \over 2}}} + {e^{{{ - 1} \over 2}}}

at x = 0

y=1+e12y = - 1 + {e^{{{ - 1} \over 2}}}
y(0)=1+e12(y(0)+1)2=e1\Rightarrow y(0) = - 1 + {e^{{{ - 1} \over 2}}} \Rightarrow {(y(0) + 1)^2} = {e^{ - 1}}
Q67
Let y = y(x) be the solution of the differential equation dydx=1+xeyx,2<x<2,y(0)=0{{dy} \over {dx}} = 1 + x{e^{y - x}}, - \sqrt 2 < x < \sqrt 2 ,y(0) = 0 then, the minimum value of y(x),x(2,2)y(x),x \in \left( { - \sqrt 2 ,\sqrt 2 } \right) is equal to :
A (23)loge2\left( {2 - \sqrt 3 } \right) - {\log _e}2
B (2+3)+loge2\left( {2 + \sqrt 3 } \right) + {\log _e}2
C (1+3)loge(31)\left( {1 + \sqrt 3 } \right) - {\log _e}\left( {\sqrt 3 - 1} \right)
D (13)loge(31)\left( {1 - \sqrt 3 } \right) - {\log _e}\left( {\sqrt 3 - 1} \right)
Correct Answer
Option D
Solution
dydxeyx=xdx{{dy - dx} \over {{e^{y - x}}}} = xdx
dydxeyx=xdx\Rightarrow {{dy - dx} \over {{e^{y - x}}}} = xdx
exy=x22+c\Rightarrow - {e^{x - y}} = {{{x^2}} \over 2} + c

At x = 0, y = 0 \Rightarrow c = -1

exy=2x22\Rightarrow {e^{x - y}} = {{2 - {x^2}} \over 2}
y=xln(2x22)\Rightarrow y = x - \ln \left( {{{2 - {x^2}} \over 2}} \right)
dydx=1+2x2x2=2+2xx22x2\Rightarrow {{dy} \over {dx}} = 1 + {{2x} \over {2 - {x^2}}} = {{2 + 2x - {x^2}} \over {2 - {x^2}}}

So minimum value occurs at

x=13x = 1 - \sqrt 3
y(13)=(13)ln(2(423)2)y\left( {1 - \sqrt 3 } \right) = \left( {1 - \sqrt 3 } \right) - \ln \left( {{{2 - \left( {4 - 2\sqrt 3 } \right)} \over 2}} \right)
=(13)ln(31)= \left( {1 - \sqrt 3 } \right) - \ln \left( {\sqrt 3 - 1} \right)
Q68
Let y = y(x) be a solution curve of the differential equation (y+1)tan2xdx+tanxdy+ydx=0(y + 1){\tan ^2}x\,dx + \tan x\,dy + y\,dx = 0, x(0,π2)x \in \left( {0,{\pi \over 2}} \right). If limx0+xy(x)=1\mathop {\lim }\limits_{x \to 0 + } xy(x) = 1, then the value of y(π4)y\left( {{\pi \over 4}} \right) is :
A π4 - {\pi \over 4}
B π41{\pi \over 4} - 1
C π4+1{\pi \over 4} + 1
D π4{\pi \over 4}
Correct Answer
Option D
Solution
(y+1)tan2xdx+tanxdy+ydx=0(y + 1){\tan ^2}x\,dx + \tan x\,dy + y\,dx = 0

or

dydx+sec2xtanx.y=tanx{{dy} \over {dx}} + {{{{\sec }^2}x} \over {\tan x}}.y = - \tan x
IF=esec2xtanxdx=elntanx=tanxIF = {e^{\int {{{{{\sec }^2}x} \over {\tan x}}dx} }} = {e^{\ln \tan x}} = \tan x

\therefore

ytanx=tan2xdxy\tan x = - \int {{{\tan }^2}x\,dx}

or

ytanx=tanx+x+Cy\tan x = - \tan x + x + C

or

y=1+xtanx+Ctanxy = - 1 + {x \over {\tan x}} + {C \over {\tan x}}

or

limx0xy=x+x2tanx+Cxtanx=1\mathop {\lim }\limits_{x \to 0} xy = - x + {{{x^2}} \over {\tan x}} + {{Cx} \over {\tan x}} = 1

or C = 1

y(x)=cotx+xcotx1y(x) = \cot x + x\cot x - 1
y(π4)=π4y\left( {{\pi \over 4}} \right) = {\pi \over 4}
Q69
Let y(x) be the solution of the differential equation 2x2 dy + (ey - 2x)dx = 0, x > 0. If y(e) = 1, then y(1) is equal to :
A 0
B 2
C loge 2
D loge (2e)
Correct Answer
Option C
Solution
2x2dy+(ey2x)dx=02{x^2}dy + ({e^y} - 2x)dx = 0
dydx+ey2x2x2=0dydx+ey2x21x=0{{dy} \over {dx}} + {{{e^y} - 2x} \over {2{x^2}}} = 0 \Rightarrow {{dy} \over {dx}} + {{{e^y}} \over {2{x^2}}} - {1 \over x} = 0
eydydxeyx=12x2{e^{ - y}}{{dy} \over {dx}} - {{{e^{ - y}}} \over x} = - {1 \over {2{x^2}}} \Rightarrow

Put

ey=z{e^{ - y}} = z
dzdxzx=12x2xdz+zdx=dx2x{{ - dz} \over {dx}} - {z \over x} = - {1 \over {2{x^2}}} \Rightarrow xdz + zdx = {{dx} \over {2x}}
d(xz)=dx2xxz=12logex+cd(xz) = {{dx} \over {2x}} \Rightarrow xz = {1 \over 2}{\log _e}x + c
xey=12logex+cx{e^{ - y}} = {1 \over 2}{\log _e}x + c

, passes through (e, 1)

C=12\Rightarrow C = {1 \over 2}
xey=logeex2x{e^{ - y}} = {{{{\log }_e}ex} \over 2}
ey=12y=loge2{e^{ - y}} = {1 \over 2} \Rightarrow y = {\log _e}2
Q70
A differential equation representing the family of parabolas with axis parallel to y-axis and whose length of latus rectum is the distance of the point (2, -3) from the line 3x + 4y = 5, is given by :
A 10d2ydx2=1110{{{d^2}y} \over {d{x^2}}} = 11
B 11d2xdy2=1011{{{d^2}x} \over {d{y^2}}} = 10
C 10d2xdy2=1110{{{d^2}x} \over {d{y^2}}} = 11
D 11d2ydx2=1011{{{d^2}y} \over {d{x^2}}} = 10
Correct Answer
Option D
Solution

Length of latus rectum

=3(2)+4(3)55=115= {{|3(2) + 4( - 3) - 5|} \over 5} = {{11} \over 5}
(xh)2=115(yk){(x - h)^2} = {{11} \over 5}(y - k)

differentiate w.r.t. 'x' :-

2(xh)=115dydx2(x - h) = {{11} \over 5}{{dy} \over {dx}}

again differentiate

2=115d2ydx22 = {{11} \over 5}{{{d^2}y} \over {d{x^2}}}
11d2ydx2=10{{11{d^2}y} \over {d{x^2}}} = 10
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