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M. Kozlowski Physica Viva Dorrance Publishing Co, Pittsburgh, PA, USA, 2006  | 
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Papers:
 
 
(1)
 (2)
 is studied. The relaxation time 
and quantum diffusion coefficient for Planck gas are calculated. The new 
interpretation of a Planck time, 
 is 
described. It is shown that for time period shorter than 
tp the time reversal symmetry holds and for 
post-Planck time the time symmetry is broken, i.e. time arrow is 
created.
, t denotes the 
relaxation time. Due to scattering the thermal wave changes the phase in 
medium.
 
for the molecular systems is obtained with the numerical value 
Tm ~ 316 K. This 
temperature defines what is generally termed as the "room 
temperature".
.
 and 
relaxation time equals Planck time, 
 . 
The quantum of thermal energy for Planck gas, 
EPlanck=1019 GeV and quantum thermal 
diffusion coefficient DPlanck 
=(hG/c)1/2 are calculated. Within the framework of 
QHT the thermal phenomena in Planck gas can be divided into two classes, 
for time period shorter than tp the time reversal symmetry holds and for time 
period longer than tp, 
time symmetry is broken, i.e. time arrow is created.
 the quantum path has fractal dimension 
df = 2. For Dt < 
t (i.e. for attosecond laser pulses) the 
quantum particle moves on straight line with velocity 
vh which is equal the thermal wave velocity. In 
the relativistic limit vh® c the mean free path for heat carriers is 
the reduced Compton wave length 
.
.
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