Trying to solve a partial differential equation using d'Alembert's solution

jaejoon89
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Hi, I'm trying to understand this.

The given equation is y_tt = 4 y_xx
0 < x < pi, t>0
where y_tt is the 2nd derivative with respect to t, y_xx is 2nd wrt x

Boundary conditions
y(0,t) = 0 and y(pi,t) = 0

And initial conditions
y_t (x,0) = 0 = g(x)
y(x,0) = sin^2 x = f(x)

---

My teacher wrote that F(x) is the odd periodic extension of f(x), and then wrote

F(x) = sign(sinx)sin^2 x

1) I assume this is to make it odd but why wouldn't he just write sign(x)sin^2 x?

2) Also, there was a similar question in class but -infinity < x < infinity and no boundary conditions given with one of the initial conditions y(x,0) = 1/(1+x^2) = f(x). In that case, since f(x) is even why isn't it necessary to use the sign function?

Thanks for your help!
 
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jaejoon89 said:
1) I assume this is to make it odd ...
Oddness wasn't the only property he wanted.
 
Why does the sin^2 need to be corrected like that?
 
Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$ Let $$I = \int\limits_0^{\sqrt 2 / 4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx. \tag{1}$$ The representation integral of ##\arcsin## is $$\arcsin u = \int\limits_{0}^{1} \frac{\mathrm dt}{\sqrt{1-t^2}}, \qquad 0 \leqslant u \leqslant 1.$$ Plugging identity above into ##(1)## with ##u...

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