12th Grade > Mathematics
DIFFERENTIAL EQUATIONS MCQs
Total Questions : 60
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Answer: Option C. -> xy+ylogx+x sin y=C
:
C
The given equation can be written as y(1+x−1)dx+(x+logx)dy+sinydx+xcosydy=0
⇒d(y(x+logx))+d(xsiny)=0→y(x+logx)+xsiny=C
:
C
The given equation can be written as y(1+x−1)dx+(x+logx)dy+sinydx+xcosydy=0
⇒d(y(x+logx))+d(xsiny)=0→y(x+logx)+xsiny=C
Answer: Option A. -> y=C1e3x+C2e4x
:
A
The given equation can be written as (ddx−3)(dydx−4y)=0....(i)
If dydx−4y=u then (I) reduces to dudx−3u=0
⇒duu=3dx⇒u=C1e3x.Therefore, we have dydx−4y=C1e3xwhich is a linear equation whose I.F.is e−4x. So ddx(ye−4x)=C1e−x
⇒ye−4x=−C1e−x+C2⇒y=C1e3x+C2e4x
:
A
The given equation can be written as (ddx−3)(dydx−4y)=0....(i)
If dydx−4y=u then (I) reduces to dudx−3u=0
⇒duu=3dx⇒u=C1e3x.Therefore, we have dydx−4y=C1e3xwhich is a linear equation whose I.F.is e−4x. So ddx(ye−4x)=C1e−x
⇒ye−4x=−C1e−x+C2⇒y=C1e3x+C2e4x
Answer: Option D. -> sin(yx)=cx
:
D
Put y=vx.Thendydx=v+xdvdx
Given equation is dydx=vx+tanyx⇒v+xtanv⇒cotvdv=dxx⇒logsinv=logx+logc
⇒sinv=cx⇒sin(yx=cx)
:
D
Put y=vx.Thendydx=v+xdvdx
Given equation is dydx=vx+tanyx⇒v+xtanv⇒cotvdv=dxx⇒logsinv=logx+logc
⇒sinv=cx⇒sin(yx=cx)
Answer: Option B. -> 1x=cy−ylog y
:
B
dxdy+xy=x2⇒x−2dxdy+x−1y=1
Put x−1=t.Then−x−2dxdy=dtdy⇒x−2dxdy=−dtdy∴−dtdy+ty=1⇒dtdy−1yt=−1
It is linear in t. Here P=−1y.Q=−1
I.F=e∫(1y)dy=e−logy=1y
∴ Solution is t(1y)=∫(−1)1ydy=−logy+c⇒t=−ylogy+cy⇒x−1cy−ylogy.
:
B
dxdy+xy=x2⇒x−2dxdy+x−1y=1
Put x−1=t.Then−x−2dxdy=dtdy⇒x−2dxdy=−dtdy∴−dtdy+ty=1⇒dtdy−1yt=−1
It is linear in t. Here P=−1y.Q=−1
I.F=e∫(1y)dy=e−logy=1y
∴ Solution is t(1y)=∫(−1)1ydy=−logy+c⇒t=−ylogy+cy⇒x−1cy−ylogy.
Answer: Option B. -> f(yx)=cx
:
B
We have, xdy=(y+xf(yx)f′(yx))dx
⇒dydx=yx+f(yx)f′(yx)which is homogenous
Putting y=vx⇒dydx=v+xdvdx, we obtain
v+xdvdx=v+f(v)f′(v)⇒f′(v)f(v)dv=dxx
Integrating, we get log f(v)=logx+logc
⇒logf(v)=logcx⇒f(yx)=cx
:
B
We have, xdy=(y+xf(yx)f′(yx))dx
⇒dydx=yx+f(yx)f′(yx)which is homogenous
Putting y=vx⇒dydx=v+xdvdx, we obtain
v+xdvdx=v+f(v)f′(v)⇒f′(v)f(v)dv=dxx
Integrating, we get log f(v)=logx+logc
⇒logf(v)=logcx⇒f(yx)=cx
Answer: Option B. -> (x−1)3
:
B
Since f"(x)=6(x-1)
⇒f′(x)=3(x−1)2+c (integrating) ----(i)
Also, at the point (2,1), the tangent to the graph is y =3x-5and slope of thetangent = 3
⇒f′(2)=3
3(2−1)3+c=3 [from eq(i)
⇒3+c=3⇒c=0
From Eq (i) we have
f′(x)=3(x−1)2
⇒f(x)=(x−1)3+k (Integrating)----(ii)
∴1=(2−1)3+k⇒k=0
Hence the equation of the function is f(x)=(x−1)3.
:
B
Since f"(x)=6(x-1)
⇒f′(x)=3(x−1)2+c (integrating) ----(i)
Also, at the point (2,1), the tangent to the graph is y =3x-5and slope of thetangent = 3
⇒f′(2)=3
3(2−1)3+c=3 [from eq(i)
⇒3+c=3⇒c=0
From Eq (i) we have
f′(x)=3(x−1)2
⇒f(x)=(x−1)3+k (Integrating)----(ii)
∴1=(2−1)3+k⇒k=0
Hence the equation of the function is f(x)=(x−1)3.
Answer: Option B. -> x3y2+x2y=c
:
B
x2dy−2x3y3dy=3x2y4dx+2xydx⇒x2dy−2xydx=3x2y4dx+2x3y3dy⇒2xydx−x2dyy2+3x2y2dx+2x3ydy=0⇒d(x2y)+d(x3y2)=0⇒x2y+x3y2=C
:
B
x2dy−2x3y3dy=3x2y4dx+2xydx⇒x2dy−2xydx=3x2y4dx+2x3y3dy⇒2xydx−x2dyy2+3x2y2dx+2x3ydy=0⇒d(x2y)+d(x3y2)=0⇒x2y+x3y2=C
Answer: Option A. -> ellipses and hyperbolas
:
A
The given equation is linear DE and can be written as
dydx+x1−x2y=ax1−x2
Its integrating factor is e∫x1−x2dx=e−(12)log(1−x2)=1√1−x2−1<x<1 and ifx2>1then I.F.=1√x2−1
ddx(y1√1−x2)=ax(1−x2)32=−12a−2x(1−x2)32
⇒y1√1−x2=a√1−x2+C⇒y=a+C√1−x2
⇒(y−a)2=C2(1−x2)⇒(y−a)2+C2x2=C2
Thus if -1 < x < 1 the given equation represents an ellipse. If x2>1then the solution is of the form −(y−a)2+C2x2=C2which represents a hyperbola.
:
A
The given equation is linear DE and can be written as
dydx+x1−x2y=ax1−x2
Its integrating factor is e∫x1−x2dx=e−(12)log(1−x2)=1√1−x2−1<x<1 and ifx2>1then I.F.=1√x2−1
ddx(y1√1−x2)=ax(1−x2)32=−12a−2x(1−x2)32
⇒y1√1−x2=a√1−x2+C⇒y=a+C√1−x2
⇒(y−a)2=C2(1−x2)⇒(y−a)2+C2x2=C2
Thus if -1 < x < 1 the given equation represents an ellipse. If x2>1then the solution is of the form −(y−a)2+C2x2=C2which represents a hyperbola.
Answer: Option B. -> secx
:
B
The differential equation
is dydx−ytanx=−y2secxI.F.=e−∫tanxdx
This is Bernoulli's equation i.e. reducible to
linear equation.
Dividing the equation by y2, we get
1y2dydx−1ytanx=−secx............(i)
Put 1y=y⇒−1y2dydx=dYdx
Equation (i) reduces to−dydx=−ytanx=−secx⇒dYdx+Ytanx=secx, Which is a linear equation
Hence I.F.=e−∫tanxdx=secx.
:
B
The differential equation
is dydx−ytanx=−y2secxI.F.=e−∫tanxdx
This is Bernoulli's equation i.e. reducible to
linear equation.
Dividing the equation by y2, we get
1y2dydx−1ytanx=−secx............(i)
Put 1y=y⇒−1y2dydx=dYdx
Equation (i) reduces to−dydx=−ytanx=−secx⇒dYdx+Ytanx=secx, Which is a linear equation
Hence I.F.=e−∫tanxdx=secx.
Answer: Option B. -> 1x=cy−ylog y
:
B
dxdy+xy=x2⇒x−2dxdy+x−1y=1
Put x−1=t.Then−x−2dxdy=dtdy⇒x−2dxdy=−dtdy∴−dtdy+ty=1⇒dtdy−1yt=−1
It is linear in t. Here P=−1y.Q=−1
I.F=e∫(1y)dy=e−logy=1y
∴ Solution is t(1y)=∫(−1)1ydy=−logy+c⇒t=−ylogy+cy⇒x−1cy−ylogy.
:
B
dxdy+xy=x2⇒x−2dxdy+x−1y=1
Put x−1=t.Then−x−2dxdy=dtdy⇒x−2dxdy=−dtdy∴−dtdy+ty=1⇒dtdy−1yt=−1
It is linear in t. Here P=−1y.Q=−1
I.F=e∫(1y)dy=e−logy=1y
∴ Solution is t(1y)=∫(−1)1ydy=−logy+c⇒t=−ylogy+cy⇒x−1cy−ylogy.