Higher Engineering Mathematics, Sixth Edition

(Nancy Kaufman) #1

Linear first order differential equations 459


Let

3 x− 3
(x+ 1 )(x− 2 )


A
(x+ 1 )

+

B
(x− 2 )


A(x− 2 )+B(x+ 1 )
(x+ 1 )(x− 2 )
from which, 3x− 3 =A(x− 2 )+B(x+ 1 )
Whenx=−1,

− 6 =− 3 A,from which,A= 2

Whenx=2,

3 = 3 B,from which,B= 1

Hence


3 x− 3
(x+ 1 )(x− 2 )

dx

=

∫ [
2
x+ 1

+

1
x− 2

]
dx

=2ln(x+ 1 )+ln(x− 2 )

=ln[(x+ 1 )^2 (x− 2 )]

(iii) Integrating factor

e


Pdx=eln[(x+ 1 )^2 (x− 2 )]=(x+ 1 ) (^2) (x− 2 )
(iv) Substituting in equation (3) gives:
y(x+ 1 )^2 (x− 2 )



(x+ 1 )^2 (x− 2 )
1
x− 2
dx



(x+ 1 )^2 dx
(v) Hence the general solution is:
y(x+1)^2 (x−2)=^13 (x+1)^3 +c
(b) Whenx=−1,y=5 thus 5( 0 )(− 3 )= 0 +c, from
which,c=0.
Hencey(x+ 1 )^2 (x− 2 )=^13 (x+ 1 )^3
i.e.y=
(x+ 1 )^3
3 (x+ 1 )^2 (x− 2 )
and hencethe particular solution is
y=
(x+ 1 )
3 (x− 2 )
Now try the following exercise
Exercise 183 Further problemson linear
first order differential equations
In problems 1 and 2, solve the differential equa-
tions.



  1. cotx


dy
dx

= 1 − 2 y,giveny=1whenx=

π
4

.

[y=^12 +cos^2 x]


  1. t



dt

+sect(tsint+cost)θ=sect,given

t=πwhenθ=1.

[
θ=

1
t

(sint−πcost)

]


  1. Given the equation x


dy
dx

=

2
x+ 2

−y show

that the particular solution isy=

2
x

ln(x+ 2 ),
given the boundary conditions thatx=− 1
wheny=0.


  1. Show that the solution of the differential
    equation
    dy
    dx


− 2 (x+ 1 )^3 =

4
(x+ 1 )

y

is y=(x+ 1 )^4 ln(x+ 1 )^2 , given that x= 0
wheny=0.


  1. Show that the solution of the differential
    equation
    dy
    dx


+ky=asinbx

is given by:

y=

(
a
k^2 +b^2

)
(ksinbx−bcosbx)

+

(
k^2 +b^2 +ab
k^2 +b^2

)
e−kx,

giveny=1whenx=0.


  1. The equation


dv
dt

=−(av+bt),whereaand
bare constants, represents an equation of
motion when a particle moves in a resisting
medium. Solve the equation forvgiven that
v=uwhent=0.
[
v=

b
a^2


bt
a

+

(
u−

b
a^2

)
e−at

]
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