The energy converted to heat during high strain rate plastic deformati
on is measured directly using an infra-red method for Ta-2.5% W alloy
and, indirectly, using UCSD's recovery Hopkinson bar technique for the
same alloy, as well as for commercially pure Ti, 1018 steel, 6061 Al
and OFHC Cu. The infra-red measurement yields a 70% conversion of work
to heat for Ta-2.5% W and generally underestimates this factor for al
l tested materials. The final temperature at a given strain can be det
ermined indirectly, based on the calculated plastic work. For this, th
ree separate measurements are made: First, a sample is deformed at a h
igh strain rate to a total strain of, say, 60%; this is essentially an
adiabatic test. Then a second sample is deformed at the same strain r
ate to about 30% strain; this should reproduce the first half of the p
revious adiabatic stress-strain curve and in our test it does. This sa
mple is then allowed to cool down to the initial room temperature. Thi
s sample may then be heated to the temperature as was measured by the
infra-red detectors and then deformed at the same strain rate to check
if the adiabatic curve is traced. It is observed that only when the s
ample temperature is increased based on 100% conversion of the plastic
work to heat, that the original adiabatic stress-strain curve is trac
ed. It is thus concluded that the infra-red detection system records a
lower (surface) temperature than the actual temperature of the sample
. (C) 1998 Elsevier Science Ltd.