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Plenary
Lecture
Abstract: Heat treating of materials is connected
with two or three thermal equilibrium establishment and
evaluation of transition time from an initial thermal
equilibrium to another one. For example, a system of
steel components during batch quenching first is heated
to austenitizing temperature T0 (800oC – 900oC) and then
is transferred to liquid medium with temperature Tm .
After cooling in liquid is finished, the third
equilibrium establishment follows when system is
subjected to deep cryogenic treatment. In both cases
transition time is the main technological parameter
which should be properly determined to be a right
recipe. In the plenary lecture the equations for cooling
time evaluation of steel parts of any configuration are
proposed. Also, a new idea on thermal equilibrium
establishment is discussed which is based on analyzing
parabolic and hyperbolic heat conductivity equations.
According to the main postulate of thermodynamics, the
thermal equilibrium is always realized and its time of
appearing is a finite value. According to classic
parabolic heat conductivity equation, the thermal
equilibrium is established when time is infinity. The
contradiction can be solved by taking into account
thermal fluctuations which destroy exponential law of
cooling (heating) and lead to finite time of equilibrium
establishing. In the presentation, it is shown that
thermal equilibrium is realized in certain (finite) time
which depends very slightly on initial temperature and
in many cases is almost the same. However, transition
time considerably depends on size of system, its
configuration, thermal properties of material,
properties of liquid, and its agitation. The
correlations on this subject are provided to calculate
system’s transition time from one thermal equilibrium to
another. The results of investigations are used for the
new technologies development which increase wear
resistance of tools and service life of machine
components.
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