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I am trying to prove $$\int_{0}^{\infty}\frac{w^3\sin(wx)}{w^4+4} \ dw=\frac{\pi}{2}e^{-x}\cos(x), \ \ x>0$$ using an appropriate transform.

I thought of using a sine transform. The inverse of the sine transform is defined as $$\mathcal{F}^{-1}_s(F(w))=\sqrt{\frac{2}{\pi}}\int_{0}^{\infty}\sin(wx)F(w) \ dw.$$ Here, $$F(w)=\frac{w^3}{w^4+4}.$$ I thought I could prove the result by taking $$\mathcal{F}_s\left(\frac{\pi}{2}e^{-x}\cos(x)\right)=\sqrt{\frac{\pi}{2}}\int_{0}^{\infty}\sin(wx)e^{-x}\cos(x) \ dx,$$ but I do not know how to solve this integral. A hint would be great.

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    You can rewrite $\sin(\omega x) \cos(x) = [\sin((\omega+1)x) - \sin((\omega-1)x)]/2$ and integrate by parts twice. Or you can write $\sin(\cdot), \cos(\cdot)$ as the real and imaginary parts of $e^{i (\cdot) x}$. – Matthew Cassell Apr 14 '19 at 07:50
  • @Mattos I have tried to solve the integral by expressing $\sin$ and $\cos$ as exponentials. I was expecting the integral to equal $F(w)$, but I did not. I am so lost –  Apr 14 '19 at 08:54

2 Answers2

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I guess this might help. The Fourier Sine Integral is given by

$$ f(x) = \int_{0}^{\infty }B(w)\sin(wx)dw $$

where

$$ B(w) = \frac{2}{\pi}\int_{0}^{\infty }f(x)\sin(wx)dx $$

Now it is given that

$$ f(x) = \frac{\pi}{2}e^{-x}\cos(x) $$

Therefore,

$$ B(w) = \frac{2}{\pi}\int_{0}^{\infty }\frac{\pi}{2}e^{-x}\cos(x)\sin(wx)dx $$

$$ B(w) = \int_{0}^{\infty }e^{-x}\cos(x)\sin(wx)dx \hspace{1cm} ... (1) $$

Also,

$$ \sin(wx) \cos(x) = \frac{\sin((w+1)x) - \sin((w-1)x)}{2} \hspace{1cm} ... (2) $$

Now substitute (2) in (1) to get

$$ B(w) = \frac{1}{2}\left [ \int_{0}^{\infty } e^{-x} \sin((w+1)x) dx - \int_{0}^{\infty } e^{-x} \sin((w-1)x) dx \right ] $$

In order to solve the above integral, we need the following equation (more on this can be found here):

$$ \int{e^{ax}\sin({bx})dx}= \dfrac{e^{ax}}{a^{2}+b^{2}}[a\sin(bx)-b\cos(bx)] + C $$

If we substitute $a = -1$ and $b = w+1$, we get:

$$ \int_{0}^{\infty } e^{-x} \sin((w+1)x) dx = \frac{w+1}{1+(w+1)^2} $$

and when we substitute $a = -1$ and $b = w-1$, we get:

$$ \int_{0}^{\infty } e^{-x} \sin((w-1)x) dx = -\frac{w-1}{1+(w-1)^2} $$

Therefore,

$$ B(w) = \frac{1}{2}\left [ \frac{w+1}{1+(w+1)^2} + \frac{w-1}{1+(w-1)^2} \right ] = \frac{w^3}{w^4+4} $$

Thus,

$$ \int_{0}^{\infty}\frac{w^3\sin(wx)}{w^4+4} \ dw=\frac{\pi}{2}e^{-x}\cos(x) $$

Ujjwal
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0

Outline.

Expanding on @Mattos' hint, an elementary technique is to exploit the identity $2\sin A\cos B=\sin(A+B)-\sin(A-B)$ so that the indefinite integral is proportional to $I_1-I_2$ where both are proportional to $\int\frac{\sin Kx}{\exp x}\,dx$ for a constant $K$. Now use integration by parts, the first time differentiating $\sin Kx$ and integrating $\exp x$ to get an integral proportional to $\int\frac{\cos Kx}{\exp x}\,dx$. Use integration by parts a second time, differentiating $\cos Kx$ and integrating $\exp x$ to get an integral proportional to $\int\frac{\sin Kx}{\exp x}\,dx$. Notice that this is the same integral as the first one, so you can collect the integral terms to solve for $\int\frac{\sin Kx}{\exp x}\,dx$.

  • I have found this doesn't work too nicely. Integrating the second time, the $''\sin(A+B)-\sin(A-B)''$ term has different coefficients for $\sin(A+B)$ and $\sin(A-B)$. How can you simply put this to the LHS and divide by the same constant? I can only think of splitting this up in to two integrals, but this would require integration by parts four times (two for each integral). –  Apr 21 '19 at 10:48
  • @Bell What expression do you have currently? – ə̷̶̸͇̘̜́̍͗̂̄︣͟ Apr 21 '19 at 12:00