Let f ( x ) be the functional equation that satisfies x = f ( x ) e f ( x ) for all real vaues x . Find
∫ 0 e f ( x ) d x .
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Let
I
=
∫
0
e
f
(
x
)
d
x
See that
d
x
d
[
f
(
x
)
e
f
(
x
)
]
=
1
⟹
I
=
∫
0
e
d
x
d
[
f
(
x
)
e
f
(
x
)
]
f
(
x
)
Then:
I
=
∣
∣
∣
∣
0
e
f
(
x
)
2
e
f
(
x
)
−
∫
0
e
f
(
x
)
d
x
d
[
e
f
(
x
)
]
d
x
⟹
I
=
∣
∣
∣
∣
0
e
e
f
(
x
)
(
f
(
x
)
2
−
f
(
x
)
+
1
)
Now we know that when
x
=
0
,
f
(
x
)
e
f
(
x
)
=
0
Assuming that:
x
→
0
lim
f
(
x
)
=
−
∞
(or more broadly, that the function is well defined at
x
=
0
)
We also know that this implies
f
(
0
)
=
0
.
Similarly, when
x
=
e
, we know:
f
(
e
)
e
f
(
e
)
=
e
⟹
f
(
e
)
=
e
1
−
f
(
e
)
This is easily solved to yield
f
(
e
)
=
1
Plugging the numbers back into the formula for
I
, we get :
I
=
e
(
1
−
1
+
1
)
−
1
(
0
+
0
+
1
)
=
e
−
1
f ( x ) , the inverse of x e x , is known as the the Lambert W function .
It can be seen by integration by parts that
∫ 0 e f ( x ) d x = e × 1 − ∫ 0 1 x e x d x
= e − ∣ x e x − ∫ e x d x ∣ 0 1 = e − ∣ e x ( x − 1 ) ∣ 0 1
= e − 1
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Nice solution.
I don't know the Lambert function, but here is my solution:
Take f ( x ) = y :
We have the equation: x = y ⋅ e y
⇒ y x = e y ⇒ l n ( x ) − l n ( y ) = y [Taking log (base e) on both sides]
Now differentiating both sides w.r.t x , we get:
x 1 − y 1 ⋅ d x d y = d x d y
⇒ d x d y = x ( y + 1 ) y ⇒ y ⋅ d x = x ( y + 1 ) d y = y e y ( y + 1 ) d y = e y ( y 2 + y ) d y
Now, we need to find ∫ 0 e y d x = ∫ 0 1 e y ( y 2 + y ) d y
Applying Integration by Parts, we have:
∫ 0 1 e y ( y 2 + y ) d y = [ e y ( y 2 − y + 1 ) ] 0 1 = e − 1 = 1 . 7 1 8 2
\int { f(x) } =xf(x)+g(x)\\ where\quad g(x)\quad was\quad a\quad function\\ f(x)=f(x)+x\frac { d }{ dx } f(x)+\frac { dg(x) }{ dx } \\ g(x)=-\int { xdf(x) } \\ g(x)=-\int { f(x)e^{ f(x) }df(x) } \\ g(x)=-[f(x)e^{ f(x) }-e^{ f(x) }]\\ then\\ \int { f(x)dx } =xf(x)+e^{ f(x) }(1-f(x))\\ and\\ \int _{ 0 }^{ e }{ f(x)dx } =[ef(e)+e^{ f(e) }(1-f(e))]-[0f(0)+e^{ f(0) }(1-f(0))]\\ note\quad that\\ f(0)=0\quad and\quad f(e)=1\\ then\\ \int _{ 0 }^{ e }{ f(x)dx } =e-1\approx 1.71828183
d x d x = d x d ( f ( x ) e f ( x ) ) = e f ( x ) f ′ ( x ) + e f ( x ) f ′ ( x ) f ( x ) = 1
Which implies that
f 1 ( x ) 1 = e f ( x ) + e f ( x ) f ( x ) (eq.1)
Now, looking at the integral:
∫ f ( x ) d x = ∫ f ′ ( x ) f ( x ) d f ( x )
Using eq.1
∫ f ′ ( x ) f ( x ) d f ( x ) = ∫ f ( x ) 2 e f ( x ) d f ( x ) + ∫ f ( x ) e f ( x ) d f ( x )
Integrating by parts
∫ f ′ ( x ) f ( x ) d f ( x ) = ∫ f ( x ) 2 e f ( x ) d f ( x ) + ∫ f ( x ) e f ( x ) d f ( x ) = = f ( x ) 2 e f ( x ) − 2 ∫ f ( x ) e f ( x ) d f ( x ) + ∫ f ( x ) e f ( x ) d f ( x )
Integrating by parts again
f ( x ) 2 e f ( x ) − ∫ f ( x ) e f ( x ) d f ( x ) = f ( x ) 2 e f ( x ) + e f ( x ) − f ( x ) e f ( x )
Therefore:
∫ 0 e f ( x ) d x = e [ f ( e ) − 1 ] + e f ( e ) − e f ( 0 ) (eq.2)
Back to the integral:
∫ f ( x ) d x = ∫ l n ( x ) d x − ∫ l n ( f ( x ) ) d x
Using (eq.1) in the second term and using integral by parts in both terms, we find that:
∫ f ( x ) d x = x [ l n ( x ) − 1 ] + e f ( x ) [ 1 − f ( x ) l n ( f ( x ) ) ]
And therefore:
∫ 0 e f ( x ) d x = e f ( e ) − e l n ( f ( e ) ) − e f ( 0 ) (eq.3)
Using eq.2 and eq.3, we find that
f ( e ) − 1 = l n ( f ( e ) ) ⇒ f ( e ) = 1
Since e f ( 0 ) = 1 , we conclude, by eq.2 or eq.3, that
∫ 0 e f ( x ) d x = e − 1
let y=f(x) therefore, y(e)^y=x, it is an invertible function. => ∫ydx is area of y=f(x) with x-axis from x=0 to x=e which is equal to [e*1-∫xdy] where y is from 0 to 1. =e-1
If x = y e y then y = W ( x ) , where W ( x ) is the Lambert-W function.
∫ 0 e W ( x ) d x = e − 1 = 1 . 7 1 8
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I don't care if it is the Lambert W function .
x = f ( x ) e f ( x ) ⟹ f − 1 x = x e x .
I = ∫ 0 e f ( x ) d x .
Let u = f ( x ) , x = u e u .
When x = 0 , u = 0 . When x = e , u = 1 .
I = ∫ 0 1 u d x = ∫ 0 1 u d ( u e u ) .
Integration by parts:
I = [ u 2 e u ] 0 1 − ∫ 0 1 u e u d u
I = [ u 2 e u ] 0 1 − ∫ 0 1 u d ( e u )
I = [ u 2 e u ] 0 1 − [ u e u ] 0 1 + ∫ 0 1 e u d u
I = [ u 2 e u ] 0 1 − [ u e u ] 0 1 + [ e u ] 0 1
I = ( e − 0 ) − ( e − 0 ) + ( e − 1 )
I = e − 1 .