I ( n ) = ∫ 0 π ln ( 1 − 2 n cos x + n 2 ) d x
For I ( n ) as defined above, find I ( 1 0 ) I ( 1 0 0 ) ⋅ I ( 6 ) I ( 3 6 ) .
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There is a mistake in fifth line.It will be cos^2(x) not cos(x).
Nice one (+1)
Cant it be solved by simplifying the expression inside I(n) to ln[(1+ne^{ix})(1-ne^{-ix})] and using taylor series for ln(x)
We can evaluate the integrals, rather than just find relationships between them. Note that for μ > 0 , F ( μ ) = ∫ 0 π sin μ − 1 x d x = 2 μ − 1 ∫ 0 π sin μ − 1 2 1 x cos μ − 1 2 1 x d x = 2 μ ∫ 0 2 1 π sin μ − 1 x cos μ − 1 x d x = 2 μ − 1 B ( 2 1 μ , 2 1 μ ) = Γ ( μ ) 2 μ − 1 Γ ( 2 1 μ ) 2 so that F ′ ( μ ) = F ( μ ) [ ln 2 + ψ ( 2 1 μ ) − ψ ( μ ) ] and hence ∫ 0 π ln ( sin x ) d x = F ′ ( 1 ) = F ( 1 ) [ ln 2 + ψ ( 2 1 ) − ψ ( 1 ) ] = π [ ln 2 − γ − ln 4 + γ ] = − π ln 2 and hence we obtain the moderately standard integral ∫ 0 π ln ( 2 sin x ) d x = 0 If we now define I ( α ) = ∫ 0 π ln ( 1 − 2 α cos x + α 2 ) d x = 2 1 ∫ 0 2 π ln ( 1 − 2 α cos x + α 2 ) d x α ≥ 1 then I ( 1 ) = 2 1 ∫ 0 2 π ln ( 4 sin 2 2 1 x ) d x = ∫ 0 2 π ln ( 2 sin 2 1 x ) d x = 2 ∫ 0 π ln ( 2 sin x ) d x = 0 Moreover the substitution z = e i x and some contour integration yields I ′ ( α ) = 2 1 ∫ 0 2 π 1 − 2 α cos x + α 2 2 α − 2 cos x = 2 1 ∫ ∣ z ∣ = 1 1 − α ( z + z − 1 ) + α 2 2 α − z − z − 1 i z d z = − 2 i 1 ∫ ∣ z ∣ = 1 z ( z − α ) ( α z − 1 ) 2 α z − z 2 − 1 d z = − π ( R e s z = 0 + R e s z = α − 1 ) z ( z − α ) ( α z − 1 ) 2 α z − z 2 − 1 = − π ( − α 1 + α − 1 − α 1 − α − 2 ) = α 2 π for α > 1 , so that I ( α ) = I ( 1 ) + 2 π ln α = 2 π ln α α ≥ 1 so that I ( α ) I ( α 2 ) = 2 α ≥ 1 making the answer to the question equal to 4 .
Very nice! Powerful integration technique!
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It is also possible to do this by considering the electrostatic potential of an infinite charged cylindrical shell of radius 1 with constant surface charge density σ . The potential at a distance r from the axis of the cylinder is then − 2 π ε 0 σ I ( r ) for r > 1 . On the other hand, it is clear that the electrostatic potential of this cylindrical shell will only depend on this radial distance r , and hence (for r > 1 ) will be the same as that of an infinite charged line with linear charge density 2 π σ positioned along the axis of the cylinder. Thus − 2 π ε 0 σ I ( r ) = − 2 π ε 0 2 π σ ln r r > 1 and hence it follows that I ( r ) = 2 π ln r for r > 1 .
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Yeah, that's another nice way to look at it. To get LHS we integrate over the azimuth angle, and to get to RHS we can simply apply Gauss's law. Very neat!
this is new and so cool
I'm a bit busy these days . this problem is from AIITS 2 Of FIITJEE.
Try proving I(n^2)/I(n) = 2 by using a+b-x property and adding
Just saw your suggestion, sir. I did the same approach to answer it, it's below :)
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Please you are older than me . call me prakhar! :) Nice solution BTW
This integral is popularly known as Dini's integral(in honour of Italian Mathematician Ulisse Dini) and takes the values 0 for 0 < = n < 1 .And 2 π l n ( n ) for n > 1
You may also approach by writting (1-2ncos(x) + n 2 ) = (n- e x )(n- e − x )
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I ( n ) = ∫ 0 π ln ( 1 − 2 n cos ( x ) + n 2 ) d x
Since ∫ a b f ( x ) d x = ∫ a b f ( a + b − x ) d x :
I ( n ) = 2 1 [ ∫ 0 π ln ( 1 − 2 n cos ( x ) + n 2 ) d x + ∫ 0 π ln ( 1 − 2 n cos ( 0 + π − x ) + n 2 ) d x ]
I ( n ) = 2 1 [ ∫ 0 π ln ( 1 − 2 n cos ( x ) + n 2 ) d x + ∫ 0 π ln ( 1 + 2 n cos ( x ) + n 2 ) d x ]
I ( n ) = 2 1 [ ∫ 0 π ln ( 1 + 2 n 2 + n 4 − 4 n 2 cos 2 ( x ) ) d x ]
I ( n ) = 2 1 [ ∫ 0 π ln ( 1 + 2 n 2 ( 1 − 2 cos 2 ( x ) ) + n 4 ) d x ]
I ( n ) = 2 1 [ ∫ 0 π ln ( 1 − 2 n 2 cos ( 2 x ) + n 4 ) d x ]
u = 2 x → d x = 2 1 d u
I ( n ) = 4 1 [ ∫ 0 2 π ln ( 1 − 2 n 2 cos ( u ) + n 4 ) d u ]
I ( n ) = 4 1 [ ∫ 0 π ln ( 1 − 2 n 2 cos ( u ) + n 4 ) d u + ∫ π 2 π ln ( 1 − 2 n 2 cos ( u ) + n 4 ) d u ]
On second integral:
v = 2 π − u → d u = − d v
I ( n ) = 4 1 [ ∫ 0 π ln ( 1 − 2 n 2 cos ( u ) + n 4 ) d u − ∫ π 0 ln ( 1 − 2 n 2 cos ( v ) + n 4 ) d v ]
I ( n ) = 4 1 [ ∫ 0 π ln ( 1 − 2 n 2 cos ( u ) + n 4 ) d u + ∫ 0 π ln ( 1 − 2 n 2 cos ( v ) + n 4 ) d v ]
I ( n ) = 4 1 [ I ( n 2 ) + I ( n 2 ) ]
I ( n ) = 2 1 I ( n 2 )
I ( n ) I ( n 2 ) = 2
So:
I ( 1 0 ) I ( 1 0 0 ) ⋅ I ( 6 ) I ( 3 6 ) = I ( 1 0 ) I ( 1 0 2 ) ⋅ I ( 6 ) I ( 6 2 ) = 2 ⋅ 2 = 4