The concept of self-organised criticality (SOC) has recently been sugg
ested as a paradigm for the long-term behaviour of earthquakes, even t
hough many of the currently-proposed models require some tuning of the
state variables or local conservation rules to produce the universall
y-observed Gutenberg-Richter frequency-magnitude distribution with a b
value near 1. For example, a systematic negative correlation is predi
cted between model b values and the degree of conservation of local fo
rce after the slip of a single element in an elastic spring/block/fric
tional slider model. A similar relation is described here for a cellul
ar automaton model with constitutive laws based on fracture mechanics.
Such systems, although critical phenomena in the sense of producing o
rder on all scales, are clearly not universal, and may not in general
even be true examples of SOC. Nevertheless they adequately reproduce b
oth the observed power-law (fractal or multifractal) scaling and its r
eported short-term fluctuation. We also present experimental and field
evidence for similar systematic variations in b value with the degree
of force conservation (expressed in terms of a normalised crack exten
sion force) during subcritical crack growth involving the physical and
chemical influence of pore fluids during a single cycle of failure bo
th in tension and compression. We find that the level of conservation
is strongly influenced by fluid-rock interaction under stress, allowin
g energy partition into processes such as: physico-chemical stress cor
rosion reactions; the dissolution and precipitation of mineral species
on crack surfaces; and the purely mechanical phenomenon of dilatant h
ardening. All of these are known to occur in the Earth on a local scal
e, but few have been explicitly included in automaton models of seismi
city. The implication is that over long time periods pore fluids may e
xert a strong physical and chemical influence on the universal state o
f SOC which the system evolves in a complex interplay of local feedbac
k mechanisms keeping the system near criticality, perhaps most strikin
gly due to the 'valve' action of faults. In the short term, crustal fl
uids might nevertheless be responsible for systematic local fluctuatio
ns about this average state.