$\Omega\subset \mathbb{R}^N$ is a bounded smooth domain. Consider the homogeneous heat equation with zero boundary condition in $\Omega$ \begin{cases} \partial_t u-\Delta u=0 \quad(x,t)\in \Omega\times (0,T]\\ u(x,0)=u_0(x)\\ u(x,t)=0 \quad (x,t)\in \partial\Omega\times (0,T] \end{cases} Whether there is estimation like: $$ \|\nabla u(\cdot,t)\|_{L^\infty(\Omega)}\leq C\|\nabla u_0\|_{L^\infty(\Omega)}, $$ here $C$ is a constant independent of $u$ and $t$.
In fact, I wish the following estimate holds: If $u_0\in C(\bar\Omega)\cap H^1_0(\Omega)$, and satisfies that there exists $d_0>0$ and $C_0>0$ such that if $x\in \Omega$ with ${\rm dist}(x,\partial\Omega)\leq d_0$ then $$ |u_0(x)|\leq C_0{\rm dist}(x,\partial\Omega) $$ Then the solution $u(\cdot, t)$ of the heat equation will still satisfy that if $x\in \Omega$ with ${\rm dist}(x,\partial\Omega)\leq \kappa d_0$ then $$ |u(t,x)|\leq \lambda C_0{\rm dist}(x,\partial\Omega) $$ where $\kappa$ and $\lambda$ are constants only dependent on $\Omega$.