In condensed matter (liquids and solids) order can manifest itself in
the position of the atoms (this is the case in crystals) or in the ori
entation of the molecules or of the magnetizations. The forces involve
d act only over atomic distances. If the order in question is stable,
free energy is at an absolute minimum. Besides its stable state, howev
er, the system can exhibit a secondary minimum in its free energy, whi
ch often corresponds to a metastable phase. A perturbation (whether th
ermal or an external constraint) can cause the system to change from t
he metastable phase to the stable phase. The fatter initially develops
like a seed which must grow and exceed a critical size related to the
interfacial tension. When the system has a large number of metastable
states, the stable state is difficult to reach (for example in solid
friction, ferromagnetism or spin glasses). The kinetic order departs f
rom the thermodynamic equilibrium conditions. During crystal growth fl
at faces grow less quickly than rough faces. Flat dense faces develop
as growth proceeds. If the liquid contains impurities, these can becom
e concentrated at the interface, car? dissolve in the crystal and can
create dislocation walls in it. Turbulent hydrodynamic flows also exhi
bit characteristic regularities, this is the case with Benard's instab
ilities in which arrays of vortices are formed. If the instability is
increased the vortex order can become intermittent and can then lead t
o chaos.