Manage your 'e's

Calculus Level 5

I = lim k 0 1 x 2 k n = 1 k ( e x / 2 n + e x / 2 n ) d x \large I = \lim_{k\to\infty} \int_0^1 \dfrac x{2^k} \prod_{n=1}^k \left( e^{x/2^n} + e^{-x/2^n} \right) \, dx

If I I can be expressed in the form of ( e + A ) B C e \dfrac{(e+A)^B}{Ce} , where A , B A,B and C C are integers satisfying A + B + C < 5 A+B+C<5 , find the product A B C ABC .

Clarification : e 2.71828 e \approx 2.71828 denotes the Euler's number .


The answer is -4.

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2 solutions

Rishabh Jain
Jun 21, 2016

R = lim k 0 1 x 2 k n = 1 k ( e x / 2 n + e x / 2 n ) L d x \mathcal R = \lim_{k\to\infty} \int_0^1 \dfrac x{2^k} \underbrace{\prod_{n=1}^k \left( e^{x/2^n} + e^{-x/2^n} \right)}_{\mathcal L} \, dx

L = n = 1 k ( e x / 2 n + e x / 2 n ) = n = 1 k ( e x / 2 n 1 e x / 2 n 1 e x / 2 n e x / 2 n ) ( A T e l e s c o p i c P r o d u c t ) = ( e x e x e x / 2 k e x / 2 k ) \begin{aligned}\mathcal L= &\prod_{n=1}^k \left( e^{x/2^n} + e^{-x/2^n} \right)\\=&\prod_{n=1}^k \left( \dfrac{e^{x/2^{n-1}} - e^{-x/2^{n-1}}}{e^{x/2^n} - e^{-x/2^n}} \right)\\&(\color{#0C6AC7}{\mathbf{A ~Telescopic ~Product}})\\=&\left(\dfrac{e^x-e^{-x}}{e^{x/2^k} - e^{-x/2^k}}\right)\end{aligned}

R = 0 1 lim k L d x 1 x / 2 k = 0 1 lim k ( e x e x ) d x e x / 2 k 1 x / 2 k 1 e x / 2 k 1 x / 2 k 1 = 0 1 ( e x e x ) 2 d x = [ e x + e x 2 ] 0 1 = e + 1 e 2 ( e 1 e ) 2 = ( e 1 ) 2 e 2 = ( e 1 ) 2 2 e \large\begin{aligned} \mathcal R=&\displaystyle\int_0^1\displaystyle\lim_{k\to \infty}\dfrac{\mathcal{L}\mathrm{d}x}{\frac{1}{x/2^k}}\\=&\displaystyle\int_0^1\displaystyle\lim_{k\to \infty}\dfrac{(e^x-e^{-x})\mathrm{d}x}{\underbrace{\frac{e^{x/2^k}-1}{x/2^k}}_{\large 1}- \underbrace{\frac{e^{-x/2^k}-1}{x/2^k}}_{\large -1}}\\=&\Large \displaystyle\int_0^1\dfrac{(e^x-e^{-x})}{2}\mathrm{d}x\\=&\Large\left[\dfrac{e^x+e^{-x}}{2}\right]_{\large 0}^{\large 1}\\&\\=&\Large\dfrac{\overbrace{e+\frac 1e-2}^{\left(\sqrt e-\frac1{\sqrt e}\right)^2=\frac{(e-1)^2}{e}}}{2}\\=&\Large\dfrac{(e-1)^2}{2e}\end{aligned}

( 1 ) × 2 × 2 = 4 \huge\therefore~(-1)\times 2\times 2=\color{#D61F06}{\boxed{-4}}

In the second line of your simplification of R \mathcal R , you seem to be implying that e u u 1 \frac{e^u}{u} \to 1 and e u u 1 \frac{e^{-u}}{u} \to -1 as u 0 u \to 0 . Neither of these is true. What we do have is e u e u u = 2 sinh u u 2 \frac{e^u - e^{-u}}{u} = \frac{2\sinh u}{u} \to 2 as u 0 u \to 0 .

Mark Hennings - 4 years, 11 months ago

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Here, the limits are interchanged by the dominated convergence theorem where g ( x ) = sinh x g(x)=\sinh x (with the notations you used in the countour integral problem) right?

A Former Brilliant Member - 4 years, 11 months ago

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Yes, because u sinh u 1 \frac{u}{\sinh u} \le 1 for all u u .

Mark Hennings - 4 years, 11 months ago

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@Mark Hennings Yes. Thanks for confirming it!

One more thing, if we define (for natural k k ) f k ( x ) = x 2 k sinh x 2 k sinh x f_k(x)=\frac{\frac{x}{2^k}}{\sinh \frac{x}{2^k}} \sinh x (on [ 0 , 1 ] [0,1] ) and f ( x ) = sinh x f(x) = \sinh x (on [ 0 , 1 ] [0,1] ) then we can conclude that f k f f_k \to f uniformly right?

A Former Brilliant Member - 4 years, 11 months ago

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@A Former Brilliant Member Yes, that works in this case, and it is enough to enable us to interchange the limit and the integral over the finite interval [ 0 , 1 ] [0,1] .

Mark Hennings - 4 years, 11 months ago

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@Mark Hennings Yes. Thanks for confirming it (again)! (I'm very new to applying this.)

Edit:

By finite you meant bounded right?

A Former Brilliant Member - 4 years, 11 months ago

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@A Former Brilliant Member I should have said bounded.

Mark Hennings - 4 years, 11 months ago

I forgot to show + 1 1 +1-1 in my solution... Typo corrected

Rishabh Jain - 4 years, 11 months ago

@Rishabh Cool The problem asks to find the product A B C ABC , not the sum A + B + C A+B+C

Janardhanan Sivaramakrishnan - 4 years, 11 months ago

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Lol... Messed up .. Typo corrected

Rishabh Jain - 4 years, 11 months ago

We begin with the identities

-1. sinh ( 2 ϕ ) = 2 sinh ( ϕ ) cosh ( ϕ ) \sinh(2\phi ) = 2\sinh (\phi )\cosh (\phi) .

-2. cosh ( θ ) = 1 2 ( e θ + e θ ) \cosh(\theta ) = \frac{1}{2}\left ( e^{\theta}+ e^{-\theta}\right )

We have sinh ( x ) \sinh(x)

After repeatedly applying (1) k times on the above expression on each recurring hyperbolic-sine, we achieve:

sinh ( x ) = 2 k sinh ( x 2 k ) n = 1 k cosh ( x 2 k ) \sinh(x) = 2^{k}\sinh(\frac{x}{2^{k}})\prod_{n=1}^{k}\cosh(\frac{x}{2^{k}})

Now we may take the limit as k approaches infinity.

sinh ( x ) = lim k 2 k sinh ( x 2 k ) n = 1 k cosh ( x 2 k ) \sinh(x) = \lim_{k\to\infty} 2^{k}\sinh(\frac{x}{2^{k}})\prod_{n=1}^{k}\cosh(\frac{x}{2^{k}})

In order to evaluate this limit, we must define a function and use l'Hospital's Rule on the 2 k sinh ( x 2 k ) 2^{k}\sinh(\frac{x}{2^{k}}) factor.

Let (with 'a' being an arbitrary constant) f ( y ) = 2 y sinh ( a 2 y ) = sinh ( a 2 y ) 2 y f(y) = 2^{y}\sinh(\frac{a}{2^{y}}) = \frac{\sinh(\frac{a}{2^{y}})}{2^{-y}}

Using l'Hospital's Rule, we differentiate the top and bottom with respect to 'y' and easily evaluate the limit.

lim y f ( y ) = lim y ( 1 ) ( ln 2 ) ( 2 y ) ( a ) cosh ( a 2 y ) ( 1 ) ( ln 2 ) ( 2 y ) = lim y ( a ) cosh ( a 2 y ) = a cosh ( 0 ) = a \lim_{y\to\infty} f(y) =\lim_{y\to\infty} \frac{(-1)(\ln 2)(2^{-y})(a)\cosh (\frac{a}{2^{y}})}{(-1)(\ln 2)(2^{-y})} =\lim_{y\to\infty} (a)\cosh (\frac{a}{2^{y}})= a\cosh(0) = a

So,

-3. sinh ( x ) = lim k x n = 1 k cosh ( x 2 k ) \sinh(x) = \lim_{k\to\infty} x\prod_{n=1}^{k}\cosh(\frac{x}{2^{k}}) (This is essentially Viète's formula.)

Now let us look at the problem:

Using (2) the expression inside the product may be simplified to 2 cosh ( x 2 n ) 2\cosh(\frac{x}{2^{n}})

I = lim k 0 1 x 2 k n = 1 k ( 2 cosh ( x 2 n ) ) d x . I = \lim_{k\to\infty} \int_{0}^{1}\frac{x}{2^{k}}\prod_{n=1}^{k}\left (2\cosh(\frac{x}{2^{n}})\right )dx.

We now see that '2' is multiplied k times in product so it cancels with the 2^(-k) outside the product.

I = lim k 0 1 x n = 1 k ( cosh ( x 2 n ) ) d x . I = \lim_{k\to\infty} \int_{0}^{1}x\prod_{n=1}^{k}\left (\cosh(\frac{x}{2^{n}})\right )dx.

Using (3) this simplifies to a very simple integral.

I = 0 1 sinh ( x ) d x = cosh ( 1 ) cosh ( 0 ) I = \int_{0}^{1}\sinh(x)dx = \cosh(1) - \cosh(0)

To evaluate this into the correct form, we must use (2) to simplify the first term.

I = 1 2 ( e + 1 e ) 1 = e 2 + 1 2 e 1 = e 2 2 e + 1 2 e I = \frac{1}{2}(e+\frac{1}{e}) -1 = \frac{e^{2}+1}{2e} - 1 = \frac{e^{2}-2e+1}{2e}

The numerator of I I is a perfect square.

I = ( e 1 ) 2 2 e I = \frac{(e-1)^{2}}{2e} . A = 1 A=-1 , B = 2 B=2 , C = 2 C=2 .

A B C = ( 1 ) ( 2 ) ( 2 ) = -4 ABC = (-1)(2)(2) = \boxed{\textbf{-4}}

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