>
>
> In the case that the mesh lives in a higher dimensional space, you also 
> have to enforce -- either as part of the problem formulation, or as a 
> postprocess step for the output of Mesquite -- that the new nodes still 
> need to lie on the geometry as described before. In other words, nodal 
> points can move *within* the surface, but not perpendicular to it. 
>
> It is my understanding that this is precisely what Bonito et al's approach 
enforces - at least in the setting that I will be working in.  Each 
solution I obtain contains a new displacement (velocity field) *and* a new 
mean curvature of the surface.  The approach I am referring to, called 
geometric consistency, uses the identity *h* = -\laplaceBeltrami *x *to 
obtain points that lie on the new surface (at least, up to supporting the 
same mean curvature *h*).  Since I have the mean curvature of the new 
surface at each time step, I can place points x_{n+1} on the (n+1)-st 
surface according to h_{n+1} = -\lapaceBeltrami x_{n+1}, where h_{n+1} is 
an interpolation of h_n onto some new mesh, and the laplace beltrami 
operator is discretized using a mapping that is interpolated onto the new 
mesh.  This is described in the paper I attached higher up in this thread. 
I'm working on implementing this right now, but I'm not sure it will 
redistribute mesh points in tangential directions.  I think there's a 
second step to this that moves vertices around.  


  

> I have no idea whether that is possible within Mesquite, but in the 
> worst case you can always project back to the previous surface. 
>

One of the bullet points on the Mesquite page 
<https://trilinos.org/packages/mesquite/> is: **Improve surface meshes, 
adapt to surface curvature*, which at least sounds promising - I'm looking 
into that this evening.

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