Let $u\in H^1(\Omega)$ with $\nabla\times u=0$ in $\Omega\subset\mathbb{R}^3$ (open bounded domain), $u\times n=0$ on $\partial\Omega$ (where $n$ is a a normal vector to $\partial\Omega$), $\operatorname{div}(u)=0$ in $\Omega$ and $u\cdot n=0$ on $\partial\Omega$.
Prove that $u=0$.
Thanks.
For $u\in H^1(\Omega)$, you can write : \begin{equation} ||u||_{H^1(\Omega)}\leq C \{ ||u||_{L^2(\Omega)}+ ||div\ u||_{L^2(\Omega)} + ||curl\ u||_{L^2(\Omega)} + ||u\cdot n||_{H^{\frac{1}{2}}(\partial\Omega)}\} \end{equation} or, \begin{equation} ||u||_{H^1(\Omega)}\leq C \{ ||u||_{L^2(\Omega)}+ ||div\ u||_{L^2(\Omega)} + ||curl\ u||_{L^2(\Omega)} + ||u\times n||_{H^{\frac{1}{2}}(\partial\Omega)}\}. \end{equation} Now if $u\cdot n =0$ on $\partial\Omega$, then you have stronger estimate to write \begin{equation} ||u||_{H^1(\Omega)}\leq C \{ ||div\ u||_{L^2(\Omega)} + ||curl\ u||_{L^2(\Omega)}\} \end{equation} or, if $u\times n=0$ on $\partial\Omega$ then also \begin{equation} ||u||_{H^1(\Omega)}\leq C \{ ||div\ u||_{L^2(\Omega)} + ||curl\ u||_{L^2(\Omega)}\}. \end{equation}
Now, if $div\ u=curl\ u =0$ in $\Omega$ then it is straightforward to conclude $u = 0$ in $\Omega$.
Remark: The above statement holds for $u\in W^{1,p}(\Omega)$ but not necessarily for $u\in L^p(\Omega)$.
Source: (1) "On the Stokes equations with the Navier type boundary conditions": Cherif Amrouche and Nour Seloula.