Let $-\infty<a<b<+\infty$. Consider the norms $\|\cdot\|_{L^2}$, $\|\cdot\|_0$ and $\|\cdot\|_{H^1}$ defined on suitable spaces and given by
$$\|f\|_{L^2}=\left(\int_a^bf^2\right)^{\frac{1}{2}},\;\|f\|_0=\|f'\|_{L^2}\text{ and }\|f\|_{H^1}=\|f\|_{L^2}+\|f'\|_{L^2}.$$
In the book Sobolev Spaces (Robert Adams) we can see (page 184) that the norms $\|\cdot\|_0$ and $\|\cdot\|_{H^1}$ defined on $H_0^1(a,b)$ are equivalent. Hence, $H_0^1(a,b)$ equipped with the norm $\|\cdot\|_0$ is complete.
My question is: is the space $H^2(a,b)\cap H_0^1(a,b)$ equipped with the norm $\|f\|_0=\|f'\|_{L^2}$ complete?
Thanks.
The answer is No.
A similar question: Will $C[a,b]$ be complete in the norm $\|\cdot\|_{L^2}$?
(The answer will be the same No).
For your question, to construct a counterexample choose $a=0$, $b=\pi$, and take a Fourier series, say, wrt an orthogonal basis $\;\{\sin{nx}\}_{n-1}^{\infty}\;$ in $ H_0^1(0,\pi)$ $$ f(x)\overset{def}{=}\sum\limits_{n=1}^{\infty}c_n\sin{nx},\quad x\in [0,\pi],\tag{$\ast$}$$ with any coefficients $c_n$ satisfying the conditions $$\sum\limits_{n=1}^{\infty}n^2|c_n|^2<\infty,\quad \sum\limits_{n=1}^{\infty}n^4|c_n|^2=\infty.$$ Given such coefficients $c_n\,$, a function $f\in H_0^1(0,\pi)$ but $f\notin H^2(0,\pi) \cap H_0^1(0,\pi)$ due to convergence of series $(\ast)$ in the norm $\|\cdot\|_{H^1}$ and its divergence in the norm $\|\cdot\|_{H^2}\,$. Now consider a sequence of partial sums $$ f_m(x)\overset{def}{=}\sum\limits_{n=1}^{m}c_n\sin{nx},\quad x\in [0,\pi],\tag{$\ast\ast$}$$ which will be a Cauchy sequence in the norm $\|\cdot\|_{H^1}$ due to its convergence in the norm $\|\cdot\|_{H^1}$ to the element $f\in H_0^1(0,\pi)$. If the space $H^2(0,\pi)\cap H_0^1(0,\pi)$ were complete in the norm $\|\cdot\|_{H^1}\,$, the Cauchy sequence $ f_m\in H^2(0,\pi)\cap H_0^1(0,\pi)$ would converge to some element $g\in H^2(0,\pi)\cap H_0^1(0,\pi)$ which should coincide with $f\notin H^2(0,\pi)\cap H_0^1(0,\pi)$. Hence, the space $H^2(0,\pi)\cap H_0^1(0,\pi)$ cannot be complete in the norm $\|\cdot\|_{H^1}\,$.