The static and dynamic characteristics of NITINOL-reinforced composite
plates are influenced primarily by the temperature distribution insid
e the composite matrix. Such distribution arises from the electrical h
eating of NITINOL fibers embedded along the neutral plane of these com
posite plates. When temperatures are developed above the martensite tr
ansformation temperature of the NITINOL fiber, the elastic modulus of
the fibers increases approximately fourfold and significant phase reco
very forces are generated. Such thermal activation of the NITINOL fibe
rs increases the elastic energy of the fibers and enchances the stiffn
ess of the plates, provided that the phase recovery forces are high en
ough to compensate for the loss of the modulus of elasticity of the co
mposite and counterbalance the generated thermal loads. Understanding
the interaction between the thermal, static and dynamic characteristic
s of the NITINOL-reinforced plates is essential to tailoring the perfo
rmance of these plates to match changes in the operating conditions. S
uch an interaction is influenced primarily by the temperature distribu
tion inside the plates during the activation and de-activation of the
NITINOL fibers. In this study, a thermal finite element model is devel
oped to determine steady-state and transient temperature distributions
inside NITINOL-reinforced composite plates resulting from different a
ctivation strategies of the NITINOL fibers. The theoretical prediction
s are compared with experimental measurements in order to validate the
thermal finite element model. The resulting temperature distribution
can be used to determine an average modulus of elasticity of the compo
site. The average temperature rise above ambient can also be used to c
ompute the axial thermal loading on the composite plate. Such predicti
ons are utilized in computing the static and dynamic characteristics o
f NITINOL-reinforced plates which are presented in Parts II and III of
this paper, respectively.