
114 Laplace and Poisson
recall here that in the simplest form, a discrete mesh Laplacian of
a vertex f ∈ R
3
, denoted by ∆(f), is
∆(f) = f −
1
d
d
X
k=1
f
k
,
where d is the degree (number of neighbors) of the node f, and f
k
are neighbors of vertex f.
The above equation enables generalizing the principle expressed
in Equation (7.7) to irregular meshes. Setting the Laplacian ∆(f)
of a given mesh to zero while imposing some boundary conditions
leads to the construction of a minimal surface that passes through
some preset locations. The surface will look like a membrane and
have spikes around the fixed locations. On the other hand, min-
imizing the norm of ∆(f) of