engineering mathematics topic 2
TRANSCRIPT
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2 - FIRST ORDER ORDINARY DIFFERENTIAL EQUATIONS
a) Separation of Variables a!"!a! Separable)
1st Order DE can be reduced to the form )()( x f y y g = by algebraic manipulations.
Variables x and y can be separated so that x appears only on RHS and y appears only
on the HS.
!o sol"e this e#n$ integrate both sides %.r.t. x &
+= C dx x f dx dx dy
y g )()(
E'ample 1&Sol"e * =+ x y y
Solution&
+y separating "ariables$ xdx ydy * =
+y integrating both sides$ therefore the #eneral sol$tion%
E'ample ,&
Sol"ey x
y = $ -)1( =y
Solution&
+y separating "ariables$ xdx ydy =
ntegrate both sides$ the general solution %ill be&
C x y += ,,
,
1
,
1
/pply initial condition$ C += ,, 1,1
-,1
$ =C
!herefore parti&$lar sol$tion $ 0,, = x y
, 2irst Order ODE 3
C x y += ,, ,,*
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E'ample ,&
Sol"e ,, )( y xy dx dy
xy x =+
Solution&
!hat is&
xy x
y xy dx dy
+= ,
,
et vx y = $
differentiate implicitly&dx dv
x v dx dy
+= and substitute vx y = intodx dy
v v v
vx x
x v vx
xy x
y xy
+=
+=
+
1
,
,,
,,,
,
,
E#uate dx dy then&
v v v
dx dv
x v +
=+
1
,
v v
v v v v v
v v v v
dx dv
x +
=
+
=
+
=
1,
11
,,,,
Separate the "ariables
=+
dx x dv v v ,1
,
et =
+ dx
x dv
v v
,1,
C x v
v += ln,1ln
et AC ln= 7
v A x v
1lnln,ln +=+
y x A x
x y +=
lnln ,
y x
Ae xy =
&) E a&t E $ation
, 2irst Order ODE 8
y x
A x x y += lnln 2
xy
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/n e'act e#uation is al%ays in the form of )( x f y dx dy =+ %here is function of x.
!he coefficient of y is the deri"ati"e of the coefficient ofdx dy
.
4hen this is the case HS can be %ritten ( )y dx d .
E'ample 1&
Sol"e this e'act e#uation x ey x dx dy
x ,,- - =+ .
Solution&
!he e#uation can be %ritten as ( ) x ey x dx d ,- =
ntegrating both sides
+== C edx ey x x
x
,
,,-
--
,
, x C
x e
y x
+=
E'ample ,&
Sol"e 1)(sincos = y x dx
d x
Solution&
!he e#uation can be %ritten as 1))((cos =y x dx d
ntegrating both sides&
C x y x +=)(cos
So that x
C x
x y
coscos+=
,) Inte#ratin# Fa&tor
, 2irst Order ODE 0
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Steps of sol"ing 2irst order DE&
1) 4rite the e#uation in the standard form
( ) ( ) x Qy x P dx dy =+
,) 2ind the integrating factor$ ( ) x
( ) ( )[ ] = x P x e'p dx -) 9ultiply the e#uation in standard form by ( ) x and recalling that the left
hand side is :ust ( )[ ]y x dx d
$ obtain
( ) ( ) ( ) ( ) ( )
( )[ ] ( ) ( ) x Q x y x dx
d
x Q x y x x P dx dy
x
=
=+
) ntegrate the last e#uation and sol"e for y
E'ample 1&
Sol"e 1=+ x y
dx dy
Solution&
;omparing to standard 1st order linear e#uation&
x x P 1)( = and 1)( = x Q
!hen x ee x x dx
x == = ln1
)(
!herefore +== C x xdx xy ,,
2inally x C x
y +=,
E'ample&
, 2irst Order ODE *
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Sol"e -),(),( = x y dx dy
x $ 1)( =y
Solution ,&
,),(
,
1 =
x y x dx
dy
,11),ln(),ln(
===
x eeIF x x
= dx x x x y ,1
),(,
1 ,
= dx x x y ),(,1
C x
x y +
=
,),(
,1 ,
!herefore ),(,
),( - += x C x y is the #eneral sol$tion
/pply initial condition$ 1)( =y
),(,0
1 C += $ -=C
!herefore the parti&$lar sol$tion ),(6),( - += x x y
, 2irst Order ODE 1
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e) .erno$lli/s E $ation
!he e#uation is in the form nQy Py dx dy
=+
%here P and Q are function of x.
!o sol"e this e#uation$ di"ide both sides by n
y gi"es&
QPy dx dy
y nn =+ 1
et ny z = 1 $ thendx dy
y ndx dz n= )1(
9ultiply e#uation (1) by (1 n) to con"ert the first term intodx dz
&
QnPy ndx dy
y n nn
)1()1()1( 1
=+
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x y x dx
dy y = 1, 1
so that x z
x dx
dz = 1 %hich is of the form QPz dx
dz =+ that can be sol"ed by
normal
integrating factor ( 2).
x z x dx
dz = 1
2 Pdx
e $ == x dx x Pdx ln1
x x eeIF x x
11)ln(ln 1 ====
= IFdx QIF z $ = dx x x x z 11
C x dx x z +== 1
, x Cx z =
but 1= y z $ ,1 x Cx y =
!herefore 1, )( = x Cx y .
, 2irst Order ODE 1,