Differential Equations

JEE Mathematics · 179 questions · Page 8 of 18 · Click an option or "Show Solution" to reveal answer

Q71
If the solution curve of the differential equation (2x - 10y3)dy + ydx = 0, passes through the points (0, 1) and (2, β\beta), then β\beta is a root of the equation :
A y5 - 2y - 2 = 0
B 2y5 - 2y - 1 = 0
C 2y5 - y2 - 2 = 0
D y5 - y2 - 1 = 0
Correct Answer
Option D
Solution
(2x10y3)dy+ydx=0(2x - 10{y^3})dy + ydx = 0
dxdy+(2y)x=10y2\Rightarrow {{dx} \over {dy}} + \left( {{2 \over y}} \right)x = 10{y^2}
I.F.=e2ydy=e2ln(y)=y2I.F. = {e^{\int {{2 \over y}dy} }} = {e^{2\ln (y)}} = {y^2}

Solution of D.E. is \therefore

x.y=(10y2)y2.dyx\,.\,y = \int {(10{y^2}){y^2}.\,dy}
xy2=10y55+Cxy2=2y5+Cx{y^2} = {{10{y^5}} \over 5} + C \Rightarrow x{y^2} = 2{y^5} + C

It passes through (0, 1) \to 0 = 2 + C \Rightarrow C = -2 \therefore Curve is

xy2=2y52x{y^2} = 2{y^5} - 2

Now, it passes through (2, β\beta)

2β2=2β52β5β21=02{\beta ^2} = 2{\beta ^5} - 2 \Rightarrow {\beta ^5} - {\beta ^2} - 1 = 0

\therefore β\beta is root of an equation

y5y21=0{y^5} - {y^2} - 1 = 0
Q72
If dydx=2x+y2x2y{{dy} \over {dx}} = {{{2^{x + y}} - {2^x}} \over {{2^y}}}, y(0) = 1, then y(1) is equal to :
A log2(2 + e)
B log2(1 + e)
C log2(2e)
D log2(1 + e2)
Correct Answer
Option B
Solution
dydx=2x+y2x2y{{dy} \over {dx}} = {{{2^{x + y}} - {2^x}} \over {{2^y}}}
2ydydx=2x(2y1){2^y}{{dy} \over {dx}} = {2^x}({2^y} - 1)
2y2y1dy=2xdx\int {{{{2^y}} \over {{2^y} - 1}}dy = \int {{2^x}\,dx} }
ln(2y1)ln2=2xln2+C{{\ln ({2^y} - 1)} \over {\ln 2}} = {{{2^x}} \over {\ln 2}} + C
log2(2y1)=2xlog2e+C\Rightarrow {\log _2}({2^y} - 1) = {2^x}{\log _2}e + C

\because

y(0)=10=log2e+Cy(0) = 1 \Rightarrow 0 = {\log _2}e + C
C=log2eC = - {\log _2}e
log2(2y1)=(2x1)log2e\Rightarrow {\log _2}({2^y} - 1) = ({2^x} - 1){\log _2}e

put x = 1,

log2(2y1)=log2e{\log _2}({2^y} - 1) = {\log _2}e

2y = e + 1 y = log2(e + 1) Ans.

Q73
If dydx=2xy+2y.2x2x+2x+yloge2{{dy} \over {dx}} = {{{2^x}y + {2^y}{{.2}^x}} \over {{2^x} + {2^{x + y}}{{\log }_e}2}}, y(0) = 0, then for y = 1, the value of x lies in the interval :
A (1, 2)
B (12,1]\left( {{1 \over 2},1} \right]
C (2, 3)
D (0,12]\left( {0,{1 \over 2}} \right]
Correct Answer
Option A
Solution
dydx=2x(y+2y)2x(1+2yln2){{dy} \over {dx}} = {{{2^x}(y + {2^y})} \over {{2^x}(1 + {2^y}\ln 2)}}
(1+2y)ln2(y+2y)dy=dx\Rightarrow \int {{{(1 + {2^y})\ln 2} \over {(y + {2^y})}}dy = \int {dx} }
lny+2y=x+c\Rightarrow \ln \left| {y + {2^y}} \right| = x + c

x = 0; y = 0 \Rightarrow c = 0

x=lny+2y\Rightarrow x = \ln \left| {y + {2^y}} \right|

\Rightarrow at y = 1, x = ln3 \because

3(e,e2)x(1,2)3 \in (e,{e^2}) \Rightarrow x \in (1,2)
Q74
If the solution of the differential equation dydx+ex(x22)y=(x22x)(x22)e2x{{dy} \over {dx}} + {e^x}\left( {{x^2} - 2} \right)y = \left( {{x^2} - 2x} \right)\left( {{x^2} - 2} \right){e^{2x}} satisfies y(0)=0y(0) = 0, then the value of y(2) is _______________.
A -1
B 1
C 0
D e
Correct Answer
Option C
Solution

\because

dydx+ex(x22)y=(x22x)(x22)e2x{{dy} \over {dx}} + {e^x}({x^2} - 2)y = ({x^2} - 2x)({x^2} - 2){e^{2x}}

Here,

I.F.=eex(x22)dxI.F. = {e^{\int {{e^x}({x^2} - 2)dx} }}
=e(x22x)ex= {e^{({x^2} - 2x){e^x}}}

\therefore Solution of the differential equation is

y.e(x22x)ex=(x22x)(x22)e2x.e(x22x)exdxy\,.\,{e^{({x^2} - 2x){e^x}}} = \int {({x^2} - 2x)({x^2} - 2){e^{2x}}\,.\,{e^{({x^2} - 2x){e^x}}}dx}
=(x22x)ex.(x22)ex.e(x22x)exdx= \int {({x^2} - 2x){e^x}\,.\,({x^2} - 2){e^x}\,.\,{e^{({x^2} - 2x){e^x}}}dx}

Let

(x22x)ex=t({x^2} - 2x){e^x} = t

\therefore

(x22)exdx=dt({x^2} - 2){e^x}dx = dt
y.e(x22x)ex=t.etdty\,.\,{e^{({x^2} - 2x){e^x}}} = \int {t\,.\,{e^t}dt}
y.e(x22x)ex=(x22x1)e(x22x)ex+cy\,.\,{e^{({x^2} - 2x){e^x}}} = ({x^2} - 2x - 1){e^{({x^2} - 2x){e^x}}} + c

\therefore

y(0)=0y(0) = 0

\therefore

c=1c = 1

\therefore

y=(x22x1)+e(2xx2)exy = ({x^2} - 2x - 1) + {e^{(2x - {x^2}){e^x}}}

\therefore

y(2)=1+1=0y(2) = - 1 + 1 = 0
Q75
If ydydx=x[y2x2+ϕ(y2x2)ϕ(y2x2)]y{{dy} \over {dx}} = x\left[ {{{{y^2}} \over {{x^2}}} + {{\phi \left( {{{{y^2}} \over {{x^2}}}} \right)} \over {\phi '\left( {{{{y^2}} \over {{x^2}}}} \right)}}} \right], x > 0, ϕ\phi > 0, and y(1) = -1, then ϕ(y24)\phi \left( {{{{y^2}} \over 4}} \right) is equal to :
A 4 ϕ\phi (2)
B 4ϕ\phi (1)
C 2 ϕ\phi (1)
D ϕ\phi (1)
Correct Answer
Option B
Solution

Let,

y=txy = tx
dydx=t+xdtdx{{dy} \over {dx}} = t + x{{dt} \over {dx}}

\therefore

tx(t+xdtdx)=x(t2+φ(t2)φ(t2))tx\left( {t + x{{dt} \over {dx}}} \right) = x\left( {{t^2} + {{\varphi ({t^2})} \over {\varphi '({t^2})}}} \right)
t2+xtdtdx=t2+φ(t2)φ(t2){t^2} + xt{{dt} \over {dx}} = {t^2} + {{\varphi ({t^2})} \over {\varphi '({t^2})}}
tφ(t2)φ(t2)dt=dxx\int {{{t\varphi '({t^2})} \over {\varphi ({t^2})}}} dt = \int {{{dx} \over x}}

Let

φ(t2)=p\varphi ({t^2}) = p

\therefore

φ(t2)2tdt=dp\varphi '({t^2})2tdt = dp
dy2p=dxx\Rightarrow \int {{{dy} \over {2p}}} = \int {{{dx} \over x}}
12lnφ(t2)=lnx+lnc{1 \over 2}\ln \varphi ({t^2}) = \ln x + \ln c
φ(t2)=x2k\varphi ({t^2}) = {x^2}k
φ(y2x2)=kx2,φ(1)=k\varphi \left( {{{{y^2}} \over {{x^2}}}} \right) = k{x^2},\varphi (1) = k
φ(y24)=4φ(1)\varphi \left( {{{{y^2}} \over 4}} \right) = 4\varphi (1)
Q76
If y = y(x) is the solution curve of the differential equation x2dy+(y1x)dx=0{x^2}dy + \left( {y - {1 \over x}} \right)dx = 0 ; x > 0 and y(1) = 1, then y(12)y\left( {{1 \over 2}} \right) is equal to :
A 321e{3 \over 2} - {1 \over {\sqrt e }}
B 3+1e3 + {1 \over {\sqrt e }}
C 3 + e
D 3 - e
Correct Answer
Option D
Solution
x2dy+(y1x)dx=0{x^2}dy + \left( {y - {1 \over x}} \right)dx = 0

; x > 0, y(1) = 1

x2dy+(xy1)xdx=0{x^2}dy + {{(xy - 1)} \over x}dx = 0
x2dy=(xy1)xdx{x^2}dy = {{(xy - 1)} \over x}dx
dydx=1xyx3{{dy} \over {dx}} = {{1 - xy} \over {{x^3}}}
dydx=1x3yx2{{dy} \over {dx}} = {1 \over {{x^3}}} - {y \over {{x^2}}}
dydx=1x2.y=1x3{{dy} \over {dx}} = {1 \over {{x^2}}}.y = {1 \over {{x^3}}}

If

e1x2dx=e1x{e^{\int {{1 \over {{x^2}}}dx} }} = {e^{ - {1 \over x}}}
ye1x=1x3.e1xy{e^{ - {1 \over x}}} = \int {{1 \over {{x^3}}}.{e^{ - {1 \over x}}}}
ye1x=ex(1+1x)+Cy{e^{ - {1 \over x}}} = {e^{ - x}}\left( {1 + {1 \over x}} \right) + C
1.e1=e1(2)+C1.\,{e^{ - 1}} = {e^{ - 1}}(2) + C
C=e1=1eC = - {e^{ - 1}} = - {1 \over e}
ye1x=e1x(1+1x)1ey{e^{ - {1 \over x}}} = {e^{ - {1 \over x}}}\left( {1 + {1 \over x}} \right) - {1 \over e}
y(12)=31e×e2y\left( {{1 \over 2}} \right) = 3 - {1 \over e} \times {e^2}
y(12)=3ey\left( {{1 \over 2}} \right) = 3 - e
Q77
Let y = y(x) be the solution of the differential equation x(1x2)dydx+(3x2yy4x3)=0x(1 - {x^2}){{dy} \over {dx}} + (3{x^2}y - y - 4{x^3}) = 0, x>1x > 1, with y(2)=2y(2) = - 2. Then y(3) is equal to :
A -18
B -12
C -6
D -3
Correct Answer
Option A
Solution
dydx+y(3x21)x(1x2)=4x3x(1x2){{dy} \over {dx}} + {{y(3{x^2} - 1)} \over {x(1 - {x^2})}} = {{4{x^3}} \over {x(1 - {x^2})}}
IF=e3x21xx3dx=elnx3x=eln(x3x)=1x3xIF = {e^{\int {{{3{x^2} - 1} \over {x - {x^3}}}dx} }} = {e^{ - \ln |{x^3} - x|}} = {e^{ - \ln ({x^3} - x)}} = {1 \over {{x^3} - x}}

Solution of D.E. can be given by

y.1x3x=4x3x(1x2).1x(x21)dxy.\,{1 \over {{x^3} - x}} = \int {{{4{x^3}} \over {x(1 - {x^2})}}.\,{1 \over {x({x^2} - 1)}}dx}
yx3x=4x(x21)2dx\Rightarrow {y \over {{x^3} - x}} = \int {{{ - 4x} \over {{{({x^2} - 1)}^2}}}dx}
yx3x=2(x21)+c\Rightarrow {y \over {{x^3} - x}} = {2 \over {({x^2} - 1)}} + c

at x = 2, y = -2

26=23+cc=1{{ - 2} \over 6} = {2 \over 3} + c \Rightarrow c = - 1

at

x=3y24=281y=18x = 3 \Rightarrow {y \over {24}} = {2 \over 8} - 1 \Rightarrow y = - 18
Q78
Let the solution curve of the differential equation xdydxy=y2+16x2x{{dy} \over {dx}} - y = \sqrt {{y^2} + 16{x^2}} , y(1)=3y(1) = 3 be y=y(x)y = y(x). Then y(2) is equal to:
A 15
B 11
C 13
D 17
Correct Answer
Option A
Solution

Given,

xdydxy=y2+16xx{{dy} \over {dx}} - y = \sqrt {{y^2} + 16x}
xdydx=y+y2+16x\Rightarrow x{{dy} \over {dx}} = y + \sqrt {{y^2} + 16x}
dydx=yx+(yx)2+16\Rightarrow {{dy} \over {dx}} = {y \over x} + \sqrt {{{\left( {{y \over x}} \right)}^2} + 16}

This is a homogenous different equation. Let

yx=v{y \over x} = v
y=vx\Rightarrow y = vx
dydx=v+xdvdx\Rightarrow {{dy} \over {dx}} = v + x{{dv} \over {dx}}

\therefore

v+xdvdx=v+v2+16v + x{{dv} \over {dx}} =v+ \sqrt {{v^2} + 16}

\Rightarrow

xdvdx=v2+16x{{dv} \over {dx}} = \sqrt {{v^2} + 16}
dvv2+16=dxx\Rightarrow {{dv} \over {\sqrt {{v^2} + 16} }} = {{dx} \over x}

Integrating both sides, we get

dvv2+16=dxx\int {{{dv} \over {\sqrt {{v^2} + 16} }} = \int {{{dx} \over x}} }
lnv+v2+16=lnx+lnc\Rightarrow \ln \left| {v + \sqrt {{v^2} + 16} } \right| = \ln x + \ln c
v+v2+16=cx\Rightarrow v + \sqrt {{v^2} + 16} = cx

Now putting,

v=yxv = {y \over x}

, we get

yx+y2x2+16=cx{y \over x} + \sqrt {{{{y^2}} \over {{x^2}}} + 16} = cx
yx+y2+16x2x2=cx\Rightarrow {y \over x} + \sqrt {{{{y^2} + 16{x^2}} \over {{x^2}}}} = cx
y+y2+16x2=cx2\Rightarrow y + \sqrt {{y^2} + 16{x^2}} = c{x^2}

...... (1) Given,

y(1)=3y(1) = 3

\therefore When x = 1 then y = 3. Putting in equation (1) we get,

3+9+16=c.13 + \sqrt {9 + 16} = c.\,1
c=8\Rightarrow c = 8

\therefore Solution of equation,

y+y2+16x2=8x2y + \sqrt {{y^2} + 16{x^2}} = 8{x^2}

Now, y(2) means when x = 2 then y = ? \therefore

y+y2+16×4=8×4y + \sqrt {{y^2} + 16 \times 4} = 8 \times 4
y=15\Rightarrow y = 15
Q79
If y = y(x) is the solution of the differential equation (1+e2x)dydx+2(1+y2)ex=0\left( {1 + {e^{2x}}} \right){{dy} \over {dx}} + 2\left( {1 + {y^2}} \right){e^x} = 0 and y (0) = 0, then 6(y(0)+(y(loge3))2)6\left( {y'(0) + {{\left( {y\left( {{{\log }_e}\sqrt 3 } \right)} \right)}^2}} \right) is equal to
A 2
B -2
C -4
D -1
Correct Answer
Option C
Solution

Given,

(1+e2x)dydx+2(1+y2)ex=0(1 + {e^{2x}}){{dy} \over {dx}} + 2(1 + {y^2}){e^x} = 0
dydx=2(1+y2)ex1+e2x\Rightarrow {{dy} \over {dx}} = {{ - 2(1 + {y^2}){e^x}} \over {1 + {e^{2x}}}}
dy1+y2=2exdx(1+e2x)\Rightarrow \int {{{dy} \over {1 + {y^2}}} = \int {{{ - 2{e^x}dx} \over {(1 + {e^{2x}})}}} }
tan1(y)=2exdx(1+e2x)\Rightarrow {\tan ^{ - 1}}(y) = \int {{{ - 2{e^x}dx} \over {(1 + {e^{2x}})}}}

Now, Let

ex=t{e^x} = t
exdx=dt\Rightarrow {e^x}dx = dt
tan1(y)=2dt1+t2\Rightarrow {\tan ^{ - 1}}(y) = \int {{{ - 2dt} \over {1 + {t^2}}}}
tan1(y)=2tan1(t)+C\Rightarrow {\tan ^{ - 1}}(y) = - 2{\tan ^{ - 1}}(t) + C
tan1(y)=2tan1(ex)+C\Rightarrow {\tan ^{ - 1}}(y) = - 2{\tan ^{ - 1}}({e^x}) + C

[Putting value of t] Given, y(0) = 0 means when x = 0 the y = 0 \therefore

tan1(0)=2tan1(eo)+C{\tan ^{ - 1}}(0) = - 2{\tan ^{ - 1}}({e^o}) + C
0=2×π4+C\Rightarrow 0 = - 2 \times {\pi \over 4} + C
C=π2\Rightarrow C = {\pi \over 2}

\therefore

tan1(y)=2tan1(ex)+π2{\tan ^{ - 1}}(y) = 2{\tan ^{ - 1}}({e^x}) + {\pi \over 2}
y=tan(2tan1(ex)+π2)\Rightarrow y = \tan \left( { - 2{{\tan }^{ - 1}}({e^x}) + {\pi \over 2}} \right)

Differentiating both sides, we get

y=sec2(2tan1(ex)+π2)2.ex1+e2xy' = {\sec ^2}\left( { - 2{{\tan }^{ - 1}}({e^x}) + {\pi \over 2}} \right) - 2\,.\,{{{e^x}} \over {1 + {e^{2x}}}}
=sec2(2tan1(ex)+π2)×2ex1+e2x= {\sec ^2}\left( { - 2{{\tan }^{ - 1}}({e^x}) + {\pi \over 2}} \right) \times {{ - 2{e^x}} \over {1 + {e^{2x}}}}

\therefore

y(0)=sec2(2tan1(eo)+π2)×2eo1+eoy'(0) = {\sec ^2}\left( { - 2{{\tan }^{ - 1}}({e^o}) + {\pi \over 2}} \right) \times {{ - 2{e^o}} \over {1 + {e^o}}}
=sec2(2×π4+π2)×22= {\sec ^2}\left( { - 2 \times {\pi \over 4} + {\pi \over 2}} \right) \times {{ - 2} \over 2}
=sec2(0)x1= {\sec ^2}(0)x - 1
=1×1= 1 \times 1
=1= - 1

And

y(loge3)=tan(2tan1(eloge3)+π2)y\left( {\log _e^{\sqrt 3 }} \right) = \tan \left( { - 2{{\tan }^{ - 1}}\left( {{e^{\log _e^{\sqrt 3 }}}} \right) + {\pi \over 2}} \right)
=tan(2tan1(3)+π2)= \tan \left( { - 2{{\tan }^{ - 1}}(\sqrt 3 ) + {\pi \over 2}} \right)
=tan(2×π3+π2)= \tan \left( { - 2 \times {\pi \over 3} + {\pi \over 2}} \right)
=tan(π6)= \tan \left( { - {\pi \over 6}} \right)
=tan(π6)= - \tan \left( {{\pi \over 6}} \right)
=13= - {1 \over {\sqrt 3 }}

\therefore

6(y(0)+(y(loge3))2)6\left( {y'(0) + {{\left( {y(\log _e^{\sqrt 3 })} \right)}^2}} \right)
=6(1+(13)2)= 6\left( { - 1 + {{\left( {{{ - 1} \over {\sqrt 3 }}} \right)}^2}} \right)
=6(1+13)=6×23=4= 6\left( { - 1 + {1 \over 3}} \right) = 6 \times {{ - 2} \over 3} = - 4
Q80
Let x = x(y) be the solution of the differential equation 2yex/y2dx+(y24xex/y2)dy=02y\,{e^{x/{y^2}}}dx + \left( {{y^2} - 4x{e^{x/{y^2}}}} \right)dy = 0 such that x(1) = 0. Then, x(e) is equal to :
A eloge(2)e{\log _e}(2)
B eloge(2) - e{\log _e}(2)
C e2loge(2){e^2}{\log _e}(2)
D e2loge(2) - {e^2}{\log _e}(2)
Correct Answer
Option D
Solution

Given differential equation

2yexy2dx+(y24xexy2)dy=0,x(1)=02y{e^{{x \over {{y^2}}}}}dx + \left( {{y^2} - 4x{e^{{x \over {{y^2}}}}}} \right)dy = 0,\,x(1) = 0
exy2[2ydx4xdy]=y2dy\Rightarrow {e^{{x \over {{y^2}}}}}[2ydx - 4xdy] = - {y^2}dy
exy2[2y2dx4xydyy4]=1ydy\Rightarrow {e^{{x \over {{y^2}}}}}\left[ {{{2{y^2}dx - 4xydy} \over {{y^4}}}} \right] = {{ - 1} \over y}dy
2exy2d(xy2)=1ydy\Rightarrow 2{e^{{x \over {{y^2}}}}}d\left( {{x \over {{y^2}}}} \right) = - {1 \over y}dy
2exy2=lny+c\Rightarrow 2{e^{{x \over {{y^2}}}}} = - \ln y + c

...... (i) Now, using x(1) = 0, c = 2 So, for x(e), Put y = e in (i)

2exe2=1+22{e^{{x \over {{e^2}}}}} = - 1 + 2
xe2=ln(12)x(e)=e2ln2\Rightarrow {x \over {{e^2}}} = \ln \left( {{1 \over 2}} \right) \Rightarrow x(e) = - {e^2}\ln 2
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