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My question is, essentially, suppose I have two simply connected subset of $\mathbb{R}^n$, if I know that the boundaries of both are very close, how can I bound the determinant of the Jacobian between them. I can probably assume anything reasonable on $\Omega$, and possibly $\partial \Omega$.

More precisely:

Suppose I have a bounded simply connected set $\Omega \subset \mathbb{R}^2$, with a boundary $\partial \Omega$ that is as smooth as I like. Think of $\Omega$ as some kind of distorted circle. $\partial \Omega$ is parametrised by $X : [0, 2 \pi ] \rightarrow \partial \Omega$.

Suppose I also have an approximation to this, given by $\Omega_h$ where $\Omega_h$ is a polyhedral shape. It has a boundary $\partial \Omega_h$ that is parametrised by $X_h : [0, 2 \pi ] \rightarrow \partial \Omega_h$.

Since $\Omega_h$ approximates $\Omega$, we have that $\| X - X_h \|^2_{L^2 [0, 2 \pi] } \leq C_1 h^2$, where $C_1$ is a positive constant and $h$ is a small positive number that I control.

If I have a mapping $ \omega : \Omega_h \rightarrow \Omega $, let $J$ be the determinant of the Jacobian of $\omega$. Are there any theorems that state something like:

$ \| X_h - X \|^2_{L^2 [0, 2 \pi]} \leq C_1 h^2 \implies |J - 1|^2 \leq C_2 h^2 $,

where $C_2$ is once again a positive constant. Anything similar would be greatly appreciated.

Edit: Perhaps my question is more about whether such an $\omega$ exists.

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  • $\begingroup$ 1). What kind of bounds are you looking for when you write $|J-1|$? $J$ is not constant: it depends on $x\in\Omega_h$. 2). I am inclined to believe that no such bounds exist because there exist many diffeomorphisms $\Omega\to\Omega$ that are the identity on $\partial \Omega$. (Take a smooth vector field on $\Omega$ that vanishes on $\partial \Omega$. The flow of $X$ will generate many such diffeomorphisms.) $\endgroup$ Commented Nov 23, 2016 at 14:38
  • $\begingroup$ 1) Good point about $J$ not being constant, little oversight. I guess I mean something like $||J-1||^2){L^2 \Omega or \Omega_h} \leq C_2h^2$. 2) Also a good point. I guess my question is if there exists such a map $\omega$ such that the Jacobian has this property. I think it must be true, as if $\Omega$ and $\Omega_h$ are sufficiently close then the Jacobian will almost be the identity. $\endgroup$
    – Josiki
    Commented Nov 24, 2016 at 10:04

1 Answer 1

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First, since you are mapping a piecewise linear curve ($\partial\Omega_h$) onto a smooth one ($\partial\Omega$), a diffeomorphism $\omega: \Omega_h \rightarrow \Omega$ does not exist in the strong sense. What you want is a piecewise differentiable homeomorphism.

With that being said, as shown in this paper, Proposition 4.7, there exists a piecewise differentiable homeomorphism $\omega:\Omega_h \rightarrow \Omega$ that fulfils a second-order pointwise estimate

\begin{equation} \tag{1} \label{mapping} \|\omega - Id\|_{L^\infty(\Omega_h)} \leq Ch^2, \end{equation}

but its Jacobian fulfils only a first-order pointwise estimate

\begin{equation} \tag{2} \label{jacobian} \|J - 1\|_{L^\infty(\Omega_h)} \leq Ch, \end{equation}

where $J$ is the weak Jacobian, because $\omega$ is piecewise differentiable only. Estimate \eqref{jacobian} is optimal, so you cannot get a second-order pointwise estimate for the Jacobian. A quick way to see this is that you are mapping the piecewise linear curve $\partial\Omega_h$ onto the smooth one $\partial\Omega$, which is interpolation in disguise. Now, piecewise linear interpolation provides first-order accuracy for the gradients, only.

If you are happy with $L^p$, $1\leq p <+\infty$ estimates instead of $L^\infty$ in \eqref{mapping} and \eqref{jacobian}, you can improve those estimates as follows. Since the special choice of $\omega$ mentioned above is the identity everywhere on $\Omega_h$ except for a $h$-thick neighbourhood (or stripe) $S$ of the boundary $\partial \Omega_h$ (i.e. $\partial \Omega_h \subset S \subset \Omega_h$ with $\text{area}(S) \le Ch$), then it holds that

\begin{equation} \tag{3} \begin{split} \|\omega-Id\|_{L^p(\Omega_h)} &= \|\omega-Id\|_{L^p(S)} \le \text{area}(S)^{\frac{1}{p}} \|\omega-Id\|_{L^\infty(S)}\\ &= \text{area}(S)^{\frac{1}{p}}\|\omega-Id\|_{L^\infty(\Omega_h)} \le Ch^{2+\frac{1}{p}}; \end{split} \end{equation}

\begin{equation} \tag{4} \begin{split} \|J-1\|_{L^p(\Omega_h)} &= \|J-1\|_{L^p(S)} \le \text{area}(S)^{\frac{1}{p}} \|J-1\|_{L^\infty(S)}\\ &= \text{area}(S)^{\frac{1}{p}}\|J-1\|_{L^\infty(\Omega_h)} \le Ch^{1+\frac{1}{p}}. \end{split} \end{equation}

The bottom line is that $\omega$ is sufficiently close to the identity, as you correctly said in your comment.

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