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7/28/2019 LDEofOrder1
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1
Linear Differential Equationsof Order One
Chapter 2
Reference: DE by R. Marquez
1
First Order First Degree ODEs
A special class of first-order ordinary Des which is
generally a nonexact DE with special integrating
factor is a linear differential equation.
A linear DE of order one takes the form .
)()( xQxyPdx
dy dxxQdxxyPdy )()(
Derivative form
Differential form
dxxpexv )()(Whose integrating factor, v(x)
2
The General Solution
The general solution of
Is found by multiplying the integrating factor,
v(x) to each term and then solving for theexact DE formed.
3
)()( xQxyPdx
dy
dxxPdxxP edxxQdxxyPdye )()( )()(
dxxQeyeddxxPdxxP
)()()(
dxxQedxxPyedyedxxPdxxPdxxP
)()()()()(
The General Solution
Simplify the equation using
Integrating both sides will result to
Thus, the general solution is
4
dxxQxvxyvd )()()(
dxxpexv )()(
dxxQxvxyvd )()()(
CdxxQxvxyv )()()(
CdxxQxvxvy )()()( 1
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The General Solution
It is also possible that the given DE is not linear
in ybut instead linear in other variable.
Linear DE iny:
Linear DE in x:
. Linear in w:
5
CdxxQxvxvy )()()( 1
CdyyQyvyvx )()()( 1
CdttQtvtvw )()()( 1
)()( xQxyPdx
dy
)()( yQyxPdy
dx
)()( tQtwPdt
dw
Example: Find the general solution
6
xxxydx
dycossin4cos2)3 2
xxyy cos2cot)1 0)tan(sec)2 3 dyyxydx
2)1(1
)4 xxy
y
0sectan)5 yywdy
dw
xyedy
dx y sin)6
Find the particular solution
when x =1, y = 2
ify(10) =0
when x =1, y = 2
7
xyyx 212 dyyexdx y )sin4( 2
xyx
x
dy
dx
463 3
2
The Bernoullis Equation
8
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Definition
A differential equation that can be
expressed in the form
is called a Bernoullis equation (BE) in y.
9
)()( xQyxyPdxdy n
Definition
The BE
may be made linear upon multiplication of
and substitution of
10
)()( xQyxyPdx
dy n
nyn )1(
dx
dyyn
dx
dzyz nn )1(;1
The General Solution of BE
Thus, the BE becomes
The general solution of this linear DE in
z may be accomplished by the method
of linear DE of order one.
11
)()1()()1()1( 1 xQnxPnydx
dyyn nn
)()1()()1( xQnxPnzdx
dz
Example: Solve the following DE
12
23)1 xexyxyy Solution
dxdyy
dxdzyz 32 2; Let
Thus, the given DE becomes
2)13()13( xxezx
dx
dz 2
2)2( xxexzdx
dz which is linear in z
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Example: Solve the following DE
13
Continuation of Solution of Ex. 1
So that the integrating factor is2)2( x
xdxee
Thus, Cdxexeze xxx ))(2(
222
)2(2 Cdxxze x
Cxez x 22 2 yz22
2Cxey x
,
2)(1 22 xexCy
Exercise: Solve the given DEs
14
xyxydx
dy 33 sectan)1 xxyyyx ln)2 3/13/4
)124(77)3 35 xxxyyyx)1()4 531 yxxy
dy
dx
9
)52
2
xx ee
yy
dx
dy
7.
Exercise: Solve the given DEs
15
44534)6 yxxy
dy
dx 0)tancsc(2)7 2 dvvvwdww
37)8 yxyyx 4cot)9 xyx
dy
dx
7.
Differential Equations
Solvable by Simple
Substitution
16
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Sometimes the DE
may not be reducible at once to any of
the forms discussed so far. This meansthat the previous methods even how
effective they were would not work. But
if a wise change of variable would be
done, the equation could be
transformed into an equation that could
be well handled by one of the previous
methods.
17
0),(),( dyyxNdxyxMDEs Solvable by Simple Substitution
Solve the following
18
DEs Solvable by Simple Substitution
021 yxxedx
dy
w = x ydx
dw
dx
dy
dx
dy
dx
dw 11Substituting these to the given DE, we get
0211 wxedx
dw
0202 ww xedx
dwxe
dx
dw
Continuation of solution
19
DEs Solvable by Simple Substitution
But w = x y
Variable Separable DE
02 wxedx
dw
02 xdxdwe w02
xdxdwe w
Cxe w 2xyyx eCxCxe 22)(
Solve the following
20
7.
0)733()4( dyyxdxyx0)74( 2 yx
dx
dy
0)tan3(sec)3(tan 222 dyyxxdxyx 0tan25cos3 2 dyyxdxxyx
021 yxxedx
dy
xxyxdy
dxy ln)1(ln
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Solve the following
21
7.
021 1
xdx
dyey
0tan])(tan1)[(tan 222 ydydxeyyyyx x
DES WITH COEFFICIENTS
LINEAR IN TWO VARIABLES
22
DE w/ Coefficient Linear in Two Variables Consider the DE whose form is
(1)
It is noted that the coefficients ofdxand dyare both linear in the variables xandy. If
these coefficients are each equated to zero,
we obtain two equations of the lines of the
forms
and
23
0)()( 222111 dycybxadxcybxa
0111 cybxa0222 cybxa
DE w/ Coefficient Linear in Two Variables For these associated equations of the lines,
we consider the following three cases:
Case 1: If
then the graph of the associated equations
of the lines are coincident and the DE is
reducible to
kdx + dy = 0 , k is a constant (2)
24
0111 cybxa 0222 cybxa
2
1
2
1
2
1
c
c
b
b
a
a
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DE w/ Coefficient Linear in Two Variables Case 2: If
then the graph of the associated equationsof the lines are parallel and the DE is
reducible to
which can be handled by simple substitution.
25
2
1
2
1
2
1
c
c
b
b
a
a
0)()( 222122 dycybxadxcybxak
DE w/ Coefficient Linear in Two Variables Case 3: If
then the associated lines are intersecting
and the DE is reducible to homogeneous
DE using the substitution
x = u + h ; dx = du
y = w + k ; dy = dw
where (h, k) is the point of intersection of
the linear system
26
2
1
2
1
b
b
a
a
0
0
222
111
ckbha
ckbha
DE w/ Coefficient Linear in Two Variables In case the DE falls under case 3, try also to
check if it is an exact DE. If so, it is
suggested to use the method for exact DE
since it is much easier to perform.
27
Example1) Find the general solution of(x+ 2y + 6)dx
(2x+y )dy = 0
Solution
For the associated system of linear equations, wehave
The solution point of this is (h, k) = (2, 4)
If we let x= u + 2 ; dx = du and
y = w 4 ; dy = dw
then, upon substitution we obtain
(u +2w)du (2u +w)dy =0.28
02
062
kh
kh
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ExampleContinuation:
This is a homogeneous DE with
u = zw ; du = zdw + wdz
Then, by substitution, we get
(zw +2w) (zdw + wdz) (2zw + w)dw =0
(z +2) (zdw + wdz) (2z +1)dw =0
(z2 +2z 2z 1)dw + w(z +2)dz =0
(z2 1)dw + w(z +2)dz =0
29
01
22
dz
z
z
w
dw
Example
30
11
23
1
21 Cdz
zzw
dw
12321 |1|ln|1|ln||ln Czzw 1
32
21
)1(ln C
z
zw
1232
1
)1( Cez
zw
C
y
yx
yx
1
1)4(
42
3
422
)2()6( 3 yxCyx
Exercise
Solve the following differential equations.
1. (3x + y 8)dx + (x2y +2)dy =0
2. (16x +5y 6)dx + (3x + y 1)dy =0
3. (xy
2)dx + (3x + y
10)dy =0
4. (2x +3y +3)dx + (3x4y +13)dy =0
5. (3x + y 9)dx + (x4)dy =0
6. (x + y +1)dx + (xy 5)dy =0
7. (6x + y 9)dx + (x2y +5)dy =0
8. (y 1)dx2(x + y +1)dy =0
9. (3x + y 10)dx + (x +3y +2)dy =0
10.(7x + y 8)dx + (x2y +5)dy =031