J. Phys. IV France
Volume 04, Numéro C4, Avril 1994
3rd International Conference Laser M2P
Page(s) C4-274 - C4-274
3rd International Conference Laser M2P

J. Phys. IV France 04 (1994) C4-274-C4-274

DOI: 10.1051/jp4:1994467

The thermal calculation of bone tissue slash modes by laser radiation


Samara Branch of P.N. Lebedev Physical Institute of Russian Academy of Sciences, Novo-Sadovaja Str. 221, Samara 443011, Russia

Power laser application in medicine is based on the different interaction forms between coherent light flow and living biological tissue. Laser beam causes photothermal, photomechanical, photoablative and photo chemical effects on living tissues. Thermal effects : photocoagulation and vaporization, that tend to the thermal necrosis of living biotissues, are the results of the intensive IR laser radiation influence. Thermal necrosis area is determined by the sizes of the primary and secondary tissue heat damage. The primary damage zone is characterized by biotissue material vaporization and carbonization processes that occur at sufficient high temperatures exceeding the temperature of phase tissue substance transitions. The secondary heat damage zone is determined by the albumen denaturation processes within comparatively low temperatures. Thus, the final result of IR laser influence on biotissue is determined by the absorption volume, heating temperature that, in its turn, depends on the energy parameters of laser beam, influence time, thermophysical tissue characteristics. In present paper the thermal calculation of bone tissue slash modes by intensive IR laser radiation was fulfilled. The threshold energy density of IR laser radiation and depth of the primary thermal damage (vaporization) of bone tissue are obtained on the basis of the solution of the heat equation. The calculations have shown that the effective slash of bone tissue with the narrow primary tissue damage zone [MATH] 10 µm is achieved for pulsed CO2 - laser radiation with duration [MATH] 1 msec and energy density [MATH] 25 J/cm2. At such times of exposure the depth of the primary damage is minimum and composes the value of the order of laser radiation wavelength.

© EDP Sciences 1994