Cyclic deformation was applied to a copper tricrystal (TC) as well as a bic
rystal (BC) at constant axial plastic strain amplitude in the range of 1 x
10(-4) less than or equal to epsilon(pl) less than or equal to 4 x 10(-3).
The initial cyclic hardening of TC was found to be similar to that of BC at
low strain amplitudes. The cyclic hardening of TC is higher than that of B
C at higher epsilon(pl) and the distinction becomes pronounced with epsilon
(pl) increasing. The cyclic stress-strain (CSS) curve of TC is obviously hi
gher than that of BC. No matter for TC and BC specimens, sigma(s) increases
slowly with increasing epsilon(pl) and the difference between them is almo
st independent of epsilon(pl) when epsilon(pl) < 1.5 x 10(-3), sigma(s) of
TC and BC as well as the difference between them increase obviously after e
psilon(pl) > 1.5 x 10(-3). Both curves show almost no plateau. The above me
chanical behaviors are in accord with surface morphologies and simple analy
sis. Two effects of the grain boundary triple junction (TJ) on slip have be
en found: one is retardation to the primary slip at lower strain amplitudes
, the other is the activation of multiple slip systems due to the internal
stresses caused by the strain incompatibilities. Deformation bands appeared
near grain boundary for BC at higher strain amplitudes while these did not
occur for TC at the same strain amplitude. Microcracks nucleated near TJ f
or epsilon(pl) greater than 0.7 x 10(-4). (C) 1999 Elsevier Science S.A. Al
l rights reserved.