MHB What are the limits of integrals in the energy method for wave equations?

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The discussion focuses on the application of the energy method to wave equations, particularly examining the limits of integrals when transitioning from a bounded domain to an unbounded one. In the first example, the energy functional is defined over the interval (0, 1), while the second example extends to the entire real line. The integral limits for the second case are confirmed to be from negative to positive infinity. The importance of considering characteristic curves in the context of wave equations is also highlighted. Ultimately, the energy functional for the unbounded case is expressed as an integral over the entire real line.
mathmari
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Hey! :o

In my notes there is the following example about the energy method.

$$u_{tt}(x, t)-u_{xxtt}(x, t)-u_{xx}(x, t)=0, 0<x<1, t>0 \\ u(x, 0)=0 \\ u_t(x, 0)=0 \\ u_x(0, t)=0 \\ u_x(1, t)=0$$

$$\int_0^1(u_tu_{tt}-u_tu_{xxtt}-u_tu_{xx})dx=0 \tag 1$$

$$\int_0^1 u_tu_{tt}dx=\int_0^1\frac{1}{2}(u_t^2)_tdx=\frac{d}{dt}\int_0^1 \frac{1}{2}u_t^2dx$$

$$\int_0^1 u_t u_{xxtt}dx=-\int_0^1 u_{tx}u_{xtt}dx+[u_t u_{xtt}]_0^1=-\int_0^1\frac{1}{2}(u_{tx}^2)_tdx$$

$$\int_0^1 u_t u_{xx}dx=-\int_0^1 u_{tx}u_x dx+[u_t u_x]_0^1=-\frac{1}{2} \frac{d}{dt} \int_0^1 u_x^2dx$$

$$(1) \Rightarrow \frac{d}{dt}\int_0^1 \frac{1}{2}u_t^2dx+\frac{d}{dt}\frac{1}{2}\int_0^1 u_{tx}^2dx+\frac{d}{dt} \frac{1}{2} \int_0^1 u_x^2dx=0$$

The energy of the system is $$E(t)=\frac{1}{2}\int_0^1 (u_t^2(x, t)+u_{tx}^2(x, t)+u_{x}^2(x, t))dx$$
When we have the problem $$v_{tt}(x, t)-v_{xt}(x, t)=0, x \in \mathbb{R}, t>0 \\ v(x, 0)=0, x \in \mathbb{R} \\ v_t(x, 0)=0, x \in \mathbb{R}$$

which are the limits of the integral?? (Wondering) In this case $x \in \mathbb{R}$, do we have to take the integral on $\mathbb{R}$ ?? (Wondering) Or do we use the characteristic curves?? (Wondering)
 
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You've probably solved this by now but for the sake of completion, the limits of the energy functional are $-\infty$ and $\infty$. In fact, the energy is

$$E(t) = \frac{1}{2}\int_{-\infty}^\infty (v_t^2(x,t) + v_x^2(x,t))\, dx$$
 

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