The structural deformation in clays results from microscopic phenomena
involving the mechanical contact-stress change, the physico-chemical
variation of repulsive forces in expansive clays, and thermal dilatanc
y of macropores. These textural strains are associated to three plasti
c mechanisms represented by respectively the yield surfaces f(Tm), f(R
-A) and f(T). Under a thermal cycle, the sizes of interlamellar spaces
between clay platelets are not modified, hence the temperature cycle
is expected to have no effect on repulsive forces and thus the second
mechanism is not affected by temperature changes. This paper suggests
a formulation of a model of thermo-elasto-plastic behaviour of non-exp
ansive saturated clays characterised by two plastic mechanisms. The me
chanical yield surface f(Tm) of the contact-stress mechanism is based
on a modified cam-clay model; the thermal softening yield surface f(T)
is a plane separating two thermal domains. In normally consolidated c
onditions, the resulting response to an increase of temperature is com
pressive. However, in highly overconsolidated conditions, a small irre
versible dilative volumetric strain is observed when the temperature i
s above a threshold value. In intermediate conditions, the material st
arts with an expansion and tends to a compression. The constitutive mo
del combines thermo-mechanical hardening, predominant in normally cons
olidated states (NCS) and absent in overconsolidated states (OCS) wher
e the thermal softening occurs. The characterisation of the model requ
ires information about rheological parameters obtained from oedometric
and triaxial paths. Lastly, some numerical simulations of thermo-mech
anical tests on remoulded Boom, 'Bassin Parisien' and Pontida clays ar
e presented, which show satisfactory agreement between experiments and
model predictions.