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d
d
y
2
wp
=
Φ
(8)
dx
dx wp
thus giving y ( x ) after integrating twice.
7.2 METHOD
Although Eq. (6) is not verified in general, it is possible to write Eq. (1) in
exact way. To do that, let us multiply this equation by
τ
ξ =
(9)
wp
Therefore, Eq. (4) reduces to
pqr
τ
''
++=
τ
'
τ
0
(10)
which is precisely the homogeneous equation associated to Eq. (1); there-
fore, if
τ =
yx
1 ()
is one of the two independent solutions:
py
''
++=
qy
'
ry
0,
(11)
1
1
1
Eqs. (5) and (9) give:
'
y
y
y
α
=
1
,
β
=
-
1
,
ξ
=
1
(12)
w
w
w
Φ
As a consequence, Eq. (3) takes its exact version:
2
⎛⎞
d
y
d
y
y
1
1
,
⎝⎠
(13)
dx
w dx y
wp
1
and y ( x ) can be obtained after two integrations.
Equations (8) and (13) give the general solution of Eq. (1), in complete
harmony with the variation of parameters method developed by Lagrange
[2-4].
 
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