Given that y = y ( x ) , solve 2 0 1 7 x y y ′ − 2 0 1 7 x 2 ln y − e sin x cos x = 0
A:
y
=
e
x
c
+
2
0
1
7
e
sin
x
B:
y
=
e
c
x
+
2
0
1
7
x
e
sin
x
C:
y
=
e
x
c
+
2
0
1
7
x
e
sin
x
D:
y
=
e
c
x
+
2
0
1
7
x
e
sin
x
E: None of the above.
Clarification: c denotes the arbitrary constant of integration .
(This problem is part of the set Extraordinary Differential Equations .)
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Relevant wiki: First Order Differential Equations - Problem Solving
Because all terms in the ODE are a combination of functions on both x and y ( x ) let's proceed to check if the ODE is in exact form. To do so, convert the ODE into the form p ( x , y ) + q ( x , y ) y ′ = 0 where p ( x , y ) = ∂ x ∂ F and q ( x , y ) = ∂ y ∂ F for some function F = F ( x , y ) . We test if a such function F exists by checking if ∂ y ∂ p = ∂ x ∂ p .
With some work we can determine that in fact ∂ y ∂ ( − x 2 2 0 1 7 ln y − e sin x cos x ) = ∂ x ∂ x y 2 0 1 7 = − x 2 y 2 0 1 7 . Then we get ∂ x ∂ F + ∂ y ∂ F d x d y =0 which implies that the general solution to this is in the form F ( x , y ) = c where c is the arbitrary constant of integration. To obtain F ( x , y ) we integrate both p ( x , y ) and q ( x , y ) in terms of x and y respectively:
F ( x , y ) = ∫ p ( x , y ) d x + k ( y ) = x 2 0 1 7 ln y − e sin x + k ( y )
F ( x , y ) = ∫ q ( x , y ) d y + h ( x ) = x 2 0 1 7 ln y + h ( x )
By comparison of terms, h ( x ) = − e sin x and k ( y ) = 0 . We thus get:
F ( x , y ) = x 2 0 1 7 ln y − e sin x = c ′ ln y = 2 0 1 7 c ′ x + 2 0 1 7 x e sin x y = e c x + 2 0 1 7 x e sin x