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The transferred heat per unity of surface and time depends on surface temperature, on external
temperature at large distance from the surface and on the convection coefficient h .
Irradiation is the transfer related to EM emission and absorption. Exchanged heat quantity is
proportional to ΔT. The solution is thus complicated and cannot be solved analytically. Luckily, in
laser machining, this quantity is negligible with respect to conduction and convection.
Principle of energy conservation and Fourier equation
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The 1 law assures that energy in an isolated volume must be conserved:
Sensible energy
Latent energy
Considering a homogeneous part characterized by:
- negligible mass motions
- no internal sources
- no phase changes
we obtain the Fourier equation, describing temperature
variation in time and space: 2
α is the thermal diffusivity [m /s] and it is the ration between the thermal conductivity and the volumetric
heat capacity.
If internal sources are present, we need to add the term relative to the source itself, which can depend on
space and time: 2
In case of laser machining, energy sorption is mostly on the surface so no internal sources are present. By the
way, this equation allows to make some considerations about superposition principle, valid also in case of
surface sources: →
Fourier equation requires boundary conditions, according to geometry and its
time evolution: