[guided]This step starts from the compactness conclusions already established: after passing to a subsequence, the first derivatives $\partial_{x_i}u_{\varepsilon_k}$ converge weakly in $L^p(V)$ to functions $h_i\in L^p(V)$, the second derivatives $\partial_{x_i}\partial_{x_j}u_{\varepsilon_k}$ converge weakly in $L^p(V)$ to functions $g_{ij}\in L^p(V)$, and $u_{\varepsilon_k}\to u$ strongly in $L^p(V)$. We must prove that these functions are not artificial limits, but are exactly the weak derivatives of $u$. Fix a test function $\phi\in C_c^\infty(V)$. For the first derivatives, the smoothness of $u_{\varepsilon_k}$ permits classical integration by parts:
\begin{align*}
\int_V u_{\varepsilon_k}(x)\partial_{x_i}\phi(x)\,d\mathcal{L}^n(x)=-\int_V \partial_{x_i}u_{\varepsilon_k}(x)\phi(x)\,d\mathcal{L}^n(x).
\end{align*}
There is no boundary term because $\phi$ has compact support in $V$.
Now we pass to the limit on both sides. Define the Hölder conjugate exponent $p'\in(1,\infty)$ by the displayed identity
\begin{align*}
p' = \frac{p}{p-1}.
\end{align*}
Since $\partial_{x_i}\phi\in C_c^\infty(V)\subset L^{p'}(V)$ and $u_{\varepsilon_k}\to u$ strongly in $L^p(V)$, Hölder's inequality gives convergence of the left-hand side to
\begin{align*}
\int_V u(x)\partial_{x_i}\phi(x)\,d\mathcal{L}^n(x).
\end{align*}
Since $\partial_{x_i}u_{\varepsilon_k}\rightharpoonup h_i$ weakly in $L^p(V)$ and $\phi\in L^{p'}(V)$, the right-hand side converges to
\begin{align*}
-\int_V h_i(x)\phi(x)\,d\mathcal{L}^n(x).
\end{align*}
Therefore
\begin{align*}
\int_V u(x)\partial_{x_i}\phi(x)\,d\mathcal{L}^n(x)=-\int_V h_i(x)\phi(x)\,d\mathcal{L}^n(x),
\end{align*}
which is exactly the definition of $h_i=\partial_{x_i}u$ in $\mathcal{D}'(V)$.
For second derivatives, the same idea is applied with two integrations by parts. Since $u_{\varepsilon_k}$ is smooth and $\phi$ is compactly supported in $V$,
\begin{align*}
\int_V u_{\varepsilon_k}(x)\partial_{x_i}\partial_{x_j}\phi(x)\,d\mathcal{L}^n(x)=\int_V \partial_{x_i}\partial_{x_j}u_{\varepsilon_k}(x)\phi(x)\,d\mathcal{L}^n(x).
\end{align*}
The left-hand side converges by strong $L^p(V)$ convergence of $u_{\varepsilon_k}$ to $u$, because $\partial_{x_i}\partial_{x_j}\phi\in L^{p'}(V)$. The right-hand side converges by weak $L^p(V)$ convergence of $\partial_{x_i}\partial_{x_j}u_{\varepsilon_k}$ to $g_{ij}$, because $\phi\in L^{p'}(V)$. Hence
\begin{align*}
\int_V u(x)\partial_{x_i}\partial_{x_j}\phi(x)\,d\mathcal{L}^n(x)=\int_V g_{ij}(x)\phi(x)\,d\mathcal{L}^n(x).
\end{align*}
This is precisely the distributional identity $g_{ij}=\partial_{x_i}\partial_{x_j}u$ on $V$.
Thus the weak compactness argument has produced all first and second weak derivatives of $u$ as actual $L^p(V)$ functions. Together with $u\in L^p(V)$, this proves $u\in W^{2,p}(V)$.[/guided]