Proceedings of the International School of Physics "Enrico Fermi.", Volume 27N. Zanichelli, 1953 - Nuclear physics |
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Page 14
... heat conduction ( nT constant ) = ( 3.16 ) WI 1+ m W2 2kT In T dx One more remark should be made about the stresses in a moving medium . One has to distinguish whether the measurement is made from a stationary frame ( e.g. stagnation ...
... heat conduction ( nT constant ) = ( 3.16 ) WI 1+ m W2 2kT In T dx One more remark should be made about the stresses in a moving medium . One has to distinguish whether the measurement is made from a stationary frame ( e.g. stagnation ...
Page 17
... heat conduction can be applied have been established by B , heat conduction will , during C lead to uniform temperature . Then ( 5.4 ) L2 Το - TB 12 ~ L2 Aw where L is a macroscopic dimension of the vessel . Next , this subject will be ...
... heat conduction can be applied have been established by B , heat conduction will , during C lead to uniform temperature . Then ( 5.4 ) L2 Το - TB 12 ~ L2 Aw where L is a macroscopic dimension of the vessel . Next , this subject will be ...
Page 36
... heat conduction process , which leads to the fact that the diffusing excited molecules are not in equilibrium with their surroundings . This was first done by UBBELOHDE [ 57 ] who investigated heat conduction between parallel plates ...
... heat conduction process , which leads to the fact that the diffusing excited molecules are not in equilibrium with their surroundings . This was first done by UBBELOHDE [ 57 ] who investigated heat conduction between parallel plates ...
Contents
GREENSPAN Translational dispersion in gases | 73 |
J LAMB | 101 |
T A LITOVITZ Ultrasonic relaxation in liquids | 176 |
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absorption Acoust activation energy amplitude atoms attenuation Boltzmann equation calculated chain Chem CO₂ coefficient collision complex compressibility concentration constant courbe curve d'absorption density dipole dispersion dissociation distribution dyn/cm² elastic electrolytes electrons energy entropy of fusion equation equilibrium equilibrium constant experimental factor function gases given heat conduction imperfections interaction ionic atmosphere ions isotherme Journ kinetic l'équilibre lattice liquid LITOVITZ maximum Maxwell distribution mean free path measurements method modulus molecular motion obtained parameters paramètres peak peut Phys polyisobutylene polymer pressure quartz crystal range ratio reaction relaxation effects relaxation frequency relaxation processes Rendiconti S.I.F. rotation segment shear shown in Fig solution solvent sound specific heat stiffness structural temperature temps de relaxation theory thermal tion transition trempe ultrasonic valeur variation velocity vibrational viscosity volume water molecules wave