Critical Phenomena, Issue 51Melville S. Green, Società italiana di fisica |
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Page 452
... viscous drag , when a cylinder or sphere is rotated in the fluid . By far the most popular viscometer has been the capillary flow viscometer . This method is based on the law of Poiseuille which relates the viscosity to the flow rate of ...
... viscous drag , when a cylinder or sphere is rotated in the fluid . By far the most popular viscometer has been the capillary flow viscometer . This method is based on the law of Poiseuille which relates the viscosity to the flow rate of ...
Page 457
... viscosity anomaly . The anomalous behaviour of the viscosity is probably the first anomaly discovered in transport properties near critical points . A survey of the available experi- mental information on the subject is presented in ...
... viscosity anomaly . The anomalous behaviour of the viscosity is probably the first anomaly discovered in transport properties near critical points . A survey of the available experi- mental information on the subject is presented in ...
Page 469
... viscosity of argon at three different temperatures as a function of pressure in Fig . 19 . At low pressures the viscosity increases with temperature . The molecular origin of the viscosity is here entirely of a kinetic nature : the ...
... viscosity of argon at three different temperatures as a function of pressure in Fig . 19 . At low pressures the viscosity increases with temperature . The molecular origin of the viscosity is here entirely of a kinetic nature : the ...
Contents
Exponent relations and inequalities | 18 |
Lightscattering tests of equations of state | 22 |
The scaling function | 27 |
Copyright | |
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analytic anisotropy anomaly antiferromagnet assume assumption asymptotic Brillouin co-existence curve coefficients coexistence constant correlation function correlation length corresponding critical exponents critical isochore critical isotherm critical phenomena critical point critical point exponents critical region defined density derivatives determined dimensionality discussed divergence droplet dynamic scaling equation experimental expression extensive variables ferromagnet field fluctuations fluid free energy frequency Hamiltonian Heisenberg helium homogeneous function hydrodynamic integral interaction Ising model isochore Journ KADANOFF KAWASAKI lattice lecture Lett linear liquid logarithmic M. E. FISHER magnetic matrix measurements mode null space obtained order parameter phase boundary phase transition Phys potential power law predictions properties relation Rendiconti S.I.F. scaling function scaling hypothesis scattering Sect shown in Fig singularities specific heat spectrum spherical model Subsect superfluid susceptibility symmetry temperature thermodynamic tion values variables vector viscosity zero