I'm reading Evans' book about PDEs by myself and I'm trying understand the motivation for the definition of weak solutions to parabolic equations of second order on pages $373$ and $374$.
First, we do preliminary assumptions:
$U \subset \mathbb{R}^n$ is an open bounded set and $U_T := U \times (0,T]$ for some fixed $T > 0$.
We will first study the initial/boundary-value problem
$$(1) \begin{cases} u_t + Lu = f \ \text{in} \ U_T\\ u = 0 \ \text{on} \ \partial U \times [0,T]\\ u = g \ \text{on} \ U \times \{ t = 0 \} \end{cases}.$$
The letter $L$ denotes for each time $t$ a second order partial differential operator , having the divergence form
$$(2) \ Lu = - \sum_{i,j=1}^n (a^{ij}(x,t)u_{x_i})_{x_j} + \sum_{i=1}^n b^i u_{x_i} + c(x,t)u.$$
$\textbf{b. Weak solutions.}$ Mimicking the developments in $\S 6.1.2$ for elliptic equations, we consider first the case that $L$ has divergence form $(2)$ and try to find an appropriate notion of weak solution for the initial/boundary-value problem $(1)$. We assume for now that
\begin{align*} (5) \ a^{ij}, b^i, c &\in L^{\infty} (U_T) \ (i,j = 1, \cdots, n)\\ (6) \ f &\in L^2(U_T),\\ (7) \ g &\in L^2(U) \end{align*}
We also suppose $a^{ij} = a^{ji} \ (i,j = 1, \cdots, n)$.
Let us now define, by analogy with the notation introduced in Chapter $6$, the time-dependent bilinear form
$$(8) \ B[u,v;t] := \int_U \sum_{i,j=1}^n a^{ij}(\cdot,t) u_{x_i}v_{x_j} + \sum_{i=1}^n b^i(\cdot, t) u_{x_i} v + c(\cdot,t)uv dx$$
for $u,v \in H^1_0(U)$ and a.e. $0 \leq t \leq T$.
Now, the motivation:
$\textbf{Motivation for definition of weak solution.}$ To make plausible the following definition of weak solution, let us first temporarily suppose that $u = u(x,t)$ is in fact a smooth solution in parabolic setting of our problem $(1)$. We know switch our pointview, by associating with $u$ a mapping
$$\textbf{u}: [0,T] \longrightarrow H^1_0(U)$$
defined by
$$[\textbf{u}(t)](x) := u(x,t) \ (x \in U, 0 \leq t \leq T).$$
In other words, we are going consider $u$ not as a function of $x$ and $t$ together, but rather as a mapping $\textbf{u}$ of $t$ into the space $H^1_0(U)$ of functions of $x$. This point of view will greatly clarify the following presentation.
Returning to the problem $(1)$, let us similary define
$$\textbf{f}: [0,T] \longrightarrow L^2(U)$$
by
$$[\textbf{f}(t)](x) := f(x,t) \ (x \in U, 0 \leq t \leq T).$$
Then if we fix a function $v \in H^1_0(U)$, we can multiply the PDE $\frac{\partial u}{\partial t} + Lu = f$ by $v$ and integrate by parts to find
$$(9) \ (\textbf{u}',v) + B[\textbf{u},v;t] = (\textbf{f},v) \ \left( ' = \frac{d}{dt} \right)$$
for each $0 \leq t \leq T$, the pairing $(,)$ denoting the inner product of $L^2(U)$. Next, observe that
$$(10) \ u_t = g^0 + \sum_{j=1}^n g^j_{x_j} \ \text{in} \ U_T$$
for $g^0 := f - \sum_{i=1}^n b^i u_{x_i} - cu$ and $g^j := \sum_{i=1}^n a^{ij}u_{x_i}$ $(j = 1, \cdots, n)$. Consequently and the definitions from $\S 5.9.1$ imply the right-hand side of $(10)$ lies in the Sobolev space $H^{-1}(U)$, with
$$||u_t||_{H^{-1}(U)} \leq \left( \sum_{j=1}^n ||g^j||^2_{L^2(U)} \right)^{\frac{1}{2}} \leq C \left( ||u||_{H^1_0(U)} + ||f||_{L^2(U)} \right).$$
This estimate suggests it may be reasonable to look for weak solution with $\textbf{u}' \in H^{-1}(U)$ for a.e $0 \leq t \leq T$ , in which case the first term in $(9)$ can be reexpressed as $\langle \textbf{u}',v \rangle$, $\langle , \rangle$ being the pairing of $H^{-1}(U)$ and $H^1_0(U)$.
My doubt is how the inequalities above are obtained? I can't see how derive them since we not suppose $\textbf{u}' \in H^{-1}(U)$ and, therefore, we can't use the result from $\S 5.9.1$, which is a caracterization of the space $H^{-1}$.
Thanks in advance!
$$\max_{0 \leq t \leq T} ||\textbf{u}(t)||{L^2(U)} \leq C \left( ||\textbf{u}||{L^2(0,T;H^1_0(U))} + ||\textbf{u}'||_{L^2(0,T;H^{-1}(U))} \right),$$
the constant depending only on $T$, but I think this isn't help me since the estimative doesn't have $||f||_{L^2(U)}$.
– George Mar 05 '19 at 15:08$$1. |f|{L^2(U)}+c_0\sum{i=1}^n|u_{x_i}|{L^2(U)}+c_1|u|{L^2(U)} \leq |f|{L^2(U)}+c_2|u|{H_0^1(U)}$$
$$2. \left(\sum_{i=1}^nc_4\left| u_{x_i}\right|{L^2(U)}\right)^2 \leq c_5\sum{i=1}^n\left| u_{x_i}\right|_{L^2(U)}^2$$
I didn't understand the first inequality, because $|| \cdot ||{H^1_0(U)} = || \cdot ||{W^{1,2}(U)}$ and this norm involves the square root of the sum of the square of $L^2$-norms of $u$ and its weak derivatives of order $1$, but you only have the sum of these $L^2$-norms.
– George Mar 05 '19 at 18:26$$\left( \sum_{i=1}^n a_i \right)^2 \leq \sum_{i=1}^n a_i^2$$
with $a_i > 0$ real numbers for each $i = 1, \cdots, n$, but I can't see why this is true
– George Mar 05 '19 at 18:32