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8/9/2019 Differential Equations - Solved Assignments - Semester Summer 2007
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Assignment No 1 Question #1 :Answer
Given D.E is(1 ) (1) y x
dye xe
dx
It is not separable.By dividing both sides by ye
1 (2) x ydy
xe edx
1 (2) x ydy
xedx
Suppose thatz=x+y Diff w.r.t.x
1+dz dydx dx
dzdx
z xe
Equation (2) becomes
. ze dz x dx It is separable eq.
Taking integrating both side
. ze dz x dx
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sin( )( , )
sin( )
y y x
x f x y y
x x
For homogenous function
sin( )( , )
sin( )
y y x
x f x y y
x x
For substituting
(3) y vx Eq (1) can be written as
sin (2)sin
dy y v xdx x v
Differentiating Equation (3) with respect to x. we have
(4)dy dv
v xdx dx
From Eq (2) & Eq (4) we have
sinsin
dv y v xv x
dx x v
sinsin
dv vx v xv xdx x v
( sin 1)sin
dv x v vv x
dx x v
sin 1sin
dv v vv x
dx v
sin 1sin
dv v v x v
dx v
1sin
dv xdx v
1sin v dv dx
x
By integrating we have1
sin v dv dx x
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By using formula we havesin cos xdx x
cos lnv x c
cos( ) ln y y
x c wherev
x x
cos( ) ln y
x c x
Which is the required result
Question #3 :
2 2(xy -1)dx-(1-xy )dy (1)
Answer.2 2M=xy -1 & N=-(1-xy )
2 2(xy -1) & -(1-xy )
2 & 2
M N y y y y
M N xy xy
y y
2
2
(xy -1)
-1+xy =N
f M
x
f y
2
2 2
f(x,y)= (xy -1)
1f(x,y)= y ( )
2
dx
x x h y
Where h(y) is constant of integration
2 2
2
2 2
Differentiating w.r.t y
y( ( ))2
'( )
'( ) 1
f x x h y y y
x y h y
x y h y x y N
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2 2
2 2
2 2
2 2
By comparing sides
=h'(y) = -1 is independent of x
or integerating we have h(y)= -y
yf(x,y)= ( )
2y
f(x,y)=2
Hence the general solution of equation is given by
f(x.y)=c
y
2
y 2( )
x x y
x x y
x x y c
or x x y
c
Question#04:
Solve (by finding I.F) ( ) 1dy
x y ydx
Solution:
1
y ydxdy
x
dividing by x
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1(1 )
1
1 1(1 ) (1)
.
.
. (1)
1 1(1 ) ( )
( . )
int .
.
( 1)
dx x
x
x x x
x x
x x
x
dy y y
dx x xdy
ydx x x
It is linear in y
I F e
xe
I F multiplybyeq
dy xe xe y xe
dx x xd xe y e dx
Taking egrate both sides
xe y e c
e xy c
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Assignment 2
Question#01Solve the differential equation and mention the name of type of this D.E
3 23 (1) 2dy x y x y with ydx
solution:
3 2
2 2
3
' ',
3
First order Ordinary differential equation
dy x y x y
dx Nowbydividing the equationby x we get
dy y x y
dx x
2
2 2
' .' ',
3
It is a Bernoulli s equation By dividing the above equationby y then we get
dy y x
dx xy
1 2
1
2
2
2
. . . ' '
1
3
( 1) .
3
Putting t y
t y
Diff w r t x
dt dy y
dx dxThen equationbecomes
dt t x
dx xmultiply by above equation
dt t x
dx x
3
33ln
ln
33
int
.
.
1.
dx x x
x
egrating factor will be
I F e e
I F e
I F x x
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3 4
3
3
3
int
1 3 1
1
int ,
ln
1 1ln
Nowmultiplying theequationby egrating factor
dt t dx x x xd t
dx x x By egrating the above equation we get
t x C
x
x C where t x y y
3
1ln1 ( ln1 0)
21
0212
1 1ln
2
Applying initial condition
C
C
C
Therequired result is
x yx
Question#02 : Find an equation of orthogonal trajectory of the curve2( ) y x c
Solution.
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1 2
1 2
1
2
sin (0) 0,
0 cos 0 sin 0
0 .1 .0
0
sin4
Now u g boundary equation y we get
c c
c c
c
Hence the solutionbecomes y c x
2
2
2
sin 1,2
1 sin 42
1 sin 2
1 .0
1 0
.
, .
Nowu gtheboundarycondition y we get
c
c
c
This is a clear contradiction
Therefore theboundary value problemhas no solution
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Assignment 3
Question#01: Solve by the method of U.C.
22
2 3 2 2 2xd y dy
y x xedx dx
Solution:For complementary function,
2
2
2
3 2 0
the auxiliary equation is
3 2 0
2 2 0
( 2) 1( 2) 0
( 1)( 2) 0
( 1) 0 ,( 2) 0
1, 2
D D
m m
m m m
m m m
m m
m m
The roots are
The complementary solution is
x xc ecec y
221
For the particular solution of the given equation, well find the particular solution of :2223 x y y y .(2)
e x y y y 223 .(3) For (2), we assume P.I. as
2Cx Bx A y p
Cx B y p 2
C y p 2
Substituting in (2), we get22 2222632 xCx Bx ACx BCx
Or 22 2232622 x A BC xC BCx Equating the co-efficient
Therefore,C = 1
062 C B or 3 B
0232 A BC or27
A
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27
. 32
P I x x
For (3) we assume P.I.as:
2
x p
x
y x D Ex e
Dx Ex e
x x p e Ex Dxe Ex D y 22 xe Ex x E D D 22
x x p e Ex E De Ex x E D D y 222 2 xe Ex x E D E D 2422
Substituting in (3) we have:
x x x x
xee Ex Dxe Ex x E D De Ex x E D E D 2223422222
Or x x E E D 222
Therefore:02E D and 22E
Thus:1 E and 2 D
P.I. of (3) is: xe x x 22
The general solution of the given equation is:
222
21 2327
x xe x xecec yx x x
Question 2:Solve the D.E. by variation of Parameters
y"' y' cosec x Solution:
y"' y' cosec x
The function f(x) can be identified as
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f x cosec x
To find y c, at first the associated homogenous equation will be solvedmx mx 2 mx 3 mxy e ,y ' m e ,y '' m e ,y "' m e
Then the associated homogenous equation gives
3 mxm m e 0
Therefore, the auxiliary equation is3
mx
m m 0
as
e 0, x
Using the quadratic formula, roots of the auxiliary equation are
2m m 1 0
m 0, i
Hence, the complementary function y c is
c 1 2 3y c c cos x c sin x
Here
1
2
3
y 1
y cos x
y sinx
So
1 2 3
2 2
1 cos x sin x
W y ,y ,y 0 sin x cos x
0 cos x sinx
After expanding.
1 sin x cos x cos x 0 0 sin x 0 0 1
1
2 2
2 2
2 2
0 cos x sinx
W 0 sinx cos x
cosec x cosx sinx
0 sin x cos x cosx 0 cosx.cosec x sinx 0 sinx.cosec x
cos x.cosec x sin x.cosec x
cosec x cos x. sin x cosec x
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2
1 0 sinx
W 0 0 cos x
0 cosec x sinx
1 0 cosx.cosec x 0 0 0 sinx 0 0
cosx.cosec x cot x
3
1 cos x 0
W 0 sinx 0
0 cosx cosec x
1 sin x.cosec x 0 cos x 0 0 0 0 0
1
Integrating
11
22
33
Wu' cosec x
W
Wu' cot xWW
u' 1W
Gives
1
2
3
u cosec x dx
ln cosec x cot x
u cot x dx
cosxdx ln sinx
sinxu 1dx
x
The particular solution y p of non -homogenous equation will be py ln cosec x cotx ln sinx cosx xsinx
Hence the general solution of the given equation is
c p y y y
1 2 3c c cosx c sinx ln cosec x cotx ln sinx .cosx xsinx
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p
Substituting in the given differential equation , then
(A+2B) cos ( 2 ) sin 4 cos 2sin
quating coefficients , we obtain
A+2B=4
2 2these equation
A=0, B=2
thus X 2sin
t A B t t t
E
A Bsolving
1 2
'1 2 1 2
1 2
1
'1 2
2
general solution is
( ) ( cos sin ) 2 sin
( ) ( cos sin ) ( sin cos ) 2 cos
(0) 0 .1 .0 0 0
0
(0) 3 .1 .1 2 3
c p
t
t t
t
hence
x x x
x t e c t c t t
x t e c t c t e c t c t t
now we apply the boundary conditions x c c
c
x c c
c
1
sin 2sin
sin 0 t 0
sin , 2sin
sin 2sin
t
t
t
t
Steady StateTransient
the solution of the initial value problem is
x e t t
e t as
therefore
e t Transient Term t Steady State
hence
x e t t
the effect ofte transient ter
:
2
m becomes negligible for
t
-----------------------------------------------------------------------------------------------------Question#02
Solve by using Cauchy Euler method3 ' ' ' 2 ' ' ' 44 5 15 x y x y xy y x
Solution:
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3 3 2 2 4
t
2 2 2
3 3 3 2
3 2 2 4
3 2 4
( 4 5 15) (1)
x = e or t = Inx so that
( 1)( 1)( 2) 3 2
in eq(1), then we get
( 3 2 4 4 5 15)
( 7 15) (2)
t
t
x D x D xD y x
Let
xD
x D x D
Substituting
y e
or
y e
T
3 2
2
3 21 2 3
4 4 4
3 2
eq of (2) is
7 15 0
( 3)( 4 5) 0
3, 2
( cos sin ).
7 15 64 16 28 15 37The general solution of (2)is
t t c
t t t
p
hecharacteristic
or
so i
The complementry solution is
y c e e c t c t
e e e y
y
43 2
1 2 3
t
43 2
1 2 3
( cos sin ) 37Where t= Inx or x = e
[ cos( ) sin( )37
t t t e
c e e c t c t
x y c x x c Inx c Inx
-----------------------------------------------------------------------------------------------------------
Question#03Find the first four terms of a power series in x for the function secxSolution:
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2 4 6
2 4 6 2 4 6
2 4 6
2 4 6
4 6
1sec , cos 1 ...
cos 2 24 720using
1 12 24 720 2 24 720
_________________
...2 24 720
...2 4 48
______________5 7
+.24 360
As we know that
x x x x where x
xTherefore long division
x x x x x x
x x x
x x x
x x
2 4 6
4 6
6
2 4 6
5 611 ...2 24 720
..
5 5+...
24 48__________________
61...
720( ) sec
5 61sec 1 ...2 24 720
the interval of converge
x x x
x x
x
hence the power series for the function f x x is
x x x x
nce of this series is ( , ).2 2
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Assignment# 05
Question 1: Marks=10
The D.E
'' '3 0 x y y y has regular singular point at x=0. Justify your answer.
Solution:n
n = 0
' 1
nn = 0
'' 2n
n = 0
'' ' r 10
try a solution of the form y = c
Therefor y = (n + r) c
y = (n + r)(n + r - 1) c So that
xy + 3y - y = x r(r + 2)c + (k + r + 1
n r
n r
n r
We x
x
x
x
k k + 1 k
k = 0
1 2
k + 1 k
)(k + r + 3) c c x = 0
So that the indicial equation and exponent are r(r + 2) = 0 andr = 0, r = -2, respectively.Since (k + r + 1)(k + r + 3)c - c = 0,
1
k k + 1
01
012
023
3 04
1
n
k = 0, 1, 2,...It follows that when r = 0,
cc =(k + 1)(k + 3)
cc =
1.32cc
c = =2.4 2!4!
2ccc = =
3.5 3!5!c 2c
c = =4.6 4!6!
cc = , n = 1, 2 ,...
n!(n + 2)!
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01 0
n = 1
0= 0
2
k + 1 k
one series solution is
2y = c x 1 +n! (n + 2)!
2= cn!(n + 2)!when r = -2, Eq.(1) becomes.
(k - 1)(k + 1)c - c = 0 (2)But not here that we don't divi
n
n
n
Thus
x
x
Now
1 0 2 1
ded by (k -1)(k +1) immediatelysince this term is zero for k = 1. However, we use the recurrencerelation (2) for the cases k = 0 and k =1-1.1c - c = 0 and 0.2c - c = 0The latter equa 1
0
k k + 1
23
3 24
4 25
n
tion implies that c = 0 and so the former equationimplies that c = 0. We find,
cc = k = 2, 3, ...(k - 1)(k + 1)
cc =
1.3c 2c
c = =2.4 2!4!c 2c
c = =3.5 3!5!
2cIn general c = 2
-2 22 2
n = 3
, n = 3,4,5...n!(n - 2)!
2Thus y = c x x + (3)n!(n - 2)!
n x
2
1
, close inspection of (3) reveals that y is simplyconstant multiple of y . To see this, let k = n - 2 in (3). Weconclude that the method of Forbenius gives only one seriessolution of the gi
However
ven differential equation.
Question 2: Marks=5Find the general solution of the equation
2 '' ' 2 1( ) 0 (0, )25
x y xy x y on
Solution:
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2 '' ' 2 2
2 '' ' 2
2
Bessel Differential Equation isx + xy + (x - v )y = 0 (1)
1x + xy + (x - )y = 0 (2)25
Comparing eq (1) and (2), then we get1 1
v = , therefore v = 525So the general solution of eq
The y
y
1 1 2 15 5
(2) isy = C J (x) + C J (x)
Question 3: Marks=10
Solve the Bessel function in terms of 32
sin x of the J
Solution:
1 1
12
1 1 11 12 2 2
1 3 12 22
3 1 12 22
1/ 2 1/ 2
32
32
C o ns id er t ha t2
12 2
1
1
2 2( ) s in , ( ) cos
1 2 2s in cos
2 s incos
v v v
t ak in g v
v J x J x J x
x A s f o r
J x J x J x x
J x J x J x x
J x J x J x x
w e k n o w
J x x J x x x x
J x x x x x x
x J x x x x
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Assignment 6
Question#01:(2 1) 2 4
t
D x Dy
Dx Dy e
Solution.
The given differential equation is
2 2 4
-
To solve the highest derivative Dy, we eliminate the highest
derivative Dx.
Therefore, multiply the second equation with 2and then
su
t
Dx x Dy
Dx Dy e
btract from the first equation to have
2 2 4
2 2 2
----------------------------------
= 4 2
t
t
Dx x Dy
Dx Dy e
x e
Therefore, it is impossible to solve the system for the highest derivatives
of each variable.
Thus the system cannot be reduced to the linear normal form.
Hence, the system is a degenerate formation.
Question#02:Use the Gauss Jordan elimination method to solve the following system of linearalgebraic equations
1 3 4
1 2 3 4
1 2 3
1 2 3 4
5x 4x 2x 3
x x 2x x 1
4x x 2x 1
x x x x 0
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Solution:The augmented matrix of given system of linear algebraic equation is
5 0 4 2 3
1 1 2 1 1
4 1 2 0 1
1 1 1 1 0
We shall perform row operations on augmented matrix.Interchanging 1 st and 2 nd row, then we have
1 1 2 1 1
5 0 4 2 3~
4 1 2 0 1
1 1 1 1 0
2 1
1 1 2 1 10 5 6 3 2
~ R 5R4 1 2 0 1
1 1 1 1 0
3 1
1 1 2 1 1
0 5 6 3 2~ R 4R
0 5 6 4 3
1 1 1 1 0
4 1
1 1 2 1 1
0 5 6 3 2
~ R R 0 5 6 4 30 2 1 0 1
2
1 1 2 1 1
6 3 20 11
~ R 5 5 55 0 5 6 4 3
0 2 1 0 1
3 2
1 1 2 1 1
6 3 20 1
~ R 5R 5 5 50 0 0 1 1
0 2 1 0 1
Interchanging 3 rd and 4 th row
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1 1 2 1 1
6 3 20 1
~ 5 5 50 2 1 0 1
0 0 0 1 1
3 2
1 1 2 1 1
6 3 20 1
5 5 5~ R 2R7 6 1
0 05 5 5
0 0 0 1 1
3
1 1 2 1 1
6 3 20 1
5 5 5 5~ R6 17 0 0 17 7
0 0 0 1 1
4
1 1 2 1 1
6 3 20 1
5 5 5~ R6 1
0 0 17 7
0 0 0 1 1
3 4
1 1 2 1 1
6 3 20 16
~ R R 5 5 57 0 0 1 0 1
0 0 0 1 1
2 3
1 1 2 1 1
3 80 1 06
~ R R 5 55 0 0 1 0 1
0 0 0 1 1
2 4
1 1 2 1 1
0 1 0 0 13~ R R
0 0 1 0 150 0 0 1 1
1 2
1 0 2 1 0
0 1 0 0 1~ R R
0 0 1 0 1
0 0 0 1 1
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1 3
1 0 0 1 2
0 1 0 0 1~ R 2R
0 0 1 0 1
0 0 0 1 1
1 4
1 0 0 0 1
0 1 0 0 1~ R R
0 0 1 0 1
0 0 0 1 1
solution becomes
1
2
3
4
x 1x 1x 1x 1
Question#03:Find the general solution of the given system of D.E
dxx 2y
dtdy
2x ydt
Solution:
The given homogenous system of differential equations is
dx dt 1 2 xdy dt 2 1 y
So, the coefficient matrix will be
1 2A
2 1
Then, we shall find the eigenvalues and eigenvectors of the coefficient A. For that, thecharacteristics equation will be
2
2
1 2det A I 2 1
1 1 2 2
1 2 4
2 3
The characteristic equation is
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2
det A I 0
2 3 0
And for the roots of characteristic equation
2
22 3 0
3 3
1 3 0
1,3
For 1
1 1 2
2 1 2
1 1 2 k 2k 2kA I K
2 1 1 k 2k 2k
1 2 1 2
1 2 1 2
2k 2k 2k 2k 0A I K 0 0
2k 2k 2k 2k 0
As both equations represents the same equation, so
1 2
1 2
k k 0
k k
or
If we select an arbitrary value for k 2 as k 2 = -1 and subsequently k 1 = 1, then the correspondingeigenvector is
11
2
k 1K
k 1
For 3
1 1 2
2 1 2
1 3 2 k 2k 2kA I K
2 1 3 k 2k 2k
1 2 1 2
1 2 1 2
2k 2k 2k 2k 0A I K 0 0
2k 2k 2k 2k 0
Now too, as both equations represents the same equation, so 1 2
1 2
k k 0
k kor
If we select an arbitrary value for K2 as K2 = 1 and subsequently k 1 = 1, then the correspondingeigenvector is
1
22
k 1K
k 1
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Hence weve obtained 2 linearly independent solution vectors of the given homog enous systemas
t 3t
1 21 1
X e ,X e1 1
Thus the general solution of the system is
1 1 2 2
t 3t1 2
t 3t1 2
t 3t1 2
X c X c X
1 1X c e c e
1 1
c e c ex t
y t c e c e
The solution of the system is
t 3t1 2
t 3t
1 2
x t c e c e
y t c e c e