Integrating, we get
tan− +
+
(^1) ∫ 2 =
1
y dt
t
c
(Where t = ex)
⇒ tan–1y + tan–1t = c ⇒ tan–1y + tan–1(ex) = c
When x = 0, y = 1
⇒ tan–1 1 + tan–1(e^0 ) = c
or c=+=πππ
442
∴ tan−−^11 +=tan
2
yex π
This is the required solution of the given differential
equation.
- We h a v e dy
dx
+=2sinyx
This is a linear D.E. of the form
dy
dx
+=Py Q
Where, P = 2 and Q = sin x
Now, I.F.===eee∫∫Pdx^2 dx^2 x
∴ The solution is given by
yQdxc×=×I.F. ∫ I.F. +
⇒ ye^22 xx=+∫e sinx dx c
= − +
e^2 x xxc
5
( sin 2 cos )
⇒ yxxce=^1 − + −x
5
( sin 2 cos )^2
This is required solution of the given differential
equation.
- Equation of a circle with centre (0, a) and radius a is
x^2 + (y – a)^2 = a^2 or x^2 + y^2 = 2ay ...(1)
where a is a parameter.
Differentiating both sides of (1) w.r.t. x, we get
22 xy^2
dy
dx
ady
dx
ady
dx
xydy
dx
+= or =+
or a x
dy
dx
= y
⎛
⎝⎜
⎞
⎠⎟
+
...(2)
Putting the value of a from (2) in (1), we get
xy yx
dy
dx
yxyxy
dy
dx
(^22) += 2 222
⎛
⎝⎜
⎞
⎠⎟
⎧ +
⎨
⎪
⎩⎪
⎫
⎬
⎪
⎭⎪
− =
⎛
⎝⎜
⎞
⎠⎟
or ( )
or (xy)dy
dx
(^22) −− 20 xy=
This is the required differential equation.
- Let P(x, y) be an arbitrary point on the given curve.
The equation of the normal to the given curve at
(x, y) is Yy dy
dx
− =−−^1 ()Xx
It is given that the normal at every point passes
through a fixed point (α, β) (say).
Therefore, βα−y=−−dx
dy
()x
⇒ (x – α)dx + (y – β)dy = 0
Integrating both sides, we get
⇒−∫() ()xdxydyCαβ+∫ − =
⇒ ()x−α +()y−β =C
2 2
22
⇒ (x – α)^2 + (y – β)^2 = r^2 , where r^2 = 2C
Clearly, this equation represents a circle, having
centre at (α, β) and radius r.
- We h a v e dy
dx
+secxy⋅ =tanx ...(1)
This is a linear D.E. of the form dy
dx
+=Py Q.
Where, P = secx and Q = tanx
Now, I.F.==ee∫∫Pdx secxdx
= elog(secx + tanx) = secx + tanx
∴ The solution of (1) is given by
yx x⋅(sec +=tan ) ∫tan (secxx xdxc+ +tan )
=++∫(sec tanxxtan xdxc)
2
=+∫∫sec tanxxdx∫sec^2 xdx dxc−⋅^1 +
∴ y(secx + tanx) = secx + tanx – x + c
This is the required solution of the given differential
equation.
- We have (x^3 + y^3 )dy – x^2 ydx = 0
⇒ =
dy
dx
xy
xy
2
33 ...(1)
This is a homogeneous differential equation.
Put yvx dy
dx
vxdv
dx
= ⇒ =+ ...(2)
Now, differential equation (1) becomes
vxdv
dx
v
v
+=
1 +^3
⇒ =
+
− =−
+
xdv
dx
v
v
v v
113 v
4
3
⇒^1 + += 0
3
4
v
v
dv dx
x
Integrating both sides, we get
(^110)
v^4 v dv
dx
x
⎡ +
⎣⎢
⎤
⎦⎥
∫∫+=
⇒−^1 ++ =
3 v^3
log | | log | |vxc