function cdef = snyder_cuboid_2()

%% common information
cdef.name = 'genericCuboid_snyder_2';
cdef.source.title = 'Mainpulation of Crystal Shape by Cycles of Growth and Dissolution';
cdef.source.author = 'R.C. Snyder AND M. F. Doherty';
cdef.source.journalYear = 'AiChe, 2007';
cdef.source.info = 'Cuboid where only the edges are truncated.';
% isGeneric is 1 when Miller indices can be choosen from cdef.millerGeneric:
cdef.isGeneric = 0;

%% symmetry information
cdef.sym.defined = 8;
% system: orthorhombic
% Schoenflies: D_2h
% Herman-Mauguin: mmm
% Laue: mmm

%% lattice information
cdef.lat.unit_angle = 'degree';
cdef.lat.unit_length = 'angstrom';
cdef.lat.a = 1;
cdef.lat.b = 1;
cdef.lat.c = 1;
cdef.lat.alpha = 90;
cdef.lat.beta = 90;
cdef.lat.gamma = 90;

%% Miller indices
cdef.millerDefined = [1, 0, 0; 0, 1, 0; 0, 0, 1; ...
                      1, 1, 0; 1, 0, 1; 0, 1, 1];

%% Kinetic parameters
% Snyder gives some growht experiment examples. First, equal relative rates
cdef.relativeGrowthOne = [1; 1; 3; 10; 10; 10];
cdef.relativeDissolutionOne = cdef.relativeGrowthOne;
% Second, different rates for one of the facets:
cdef.relativeGrowthTwo = [1; 1; 3; 10; 10; 10];
cdef.relativeDissolutionTwo = [1; 1; 6; 10; 10; 10];

