Thermodynamic properties of liquid metal solutions in the sodium-mercury system at 200 deg C
Thermodynamic properties of liquid metal solutions in sodium-mercury system at high temperature
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Thermodynamic properties of liquid metal solutions in sodium-mercury system at high temperature
Some of the thermodynamic properties of liquid cobalt and palladium investigated by means of levitation calorimetry are reported and discussed. The presented data include the specific heats and heats of fusion of the liquid metals, and the emissivities of the liquid metal surfaces.
The thermodynamic properties of (CO2)N molecular aggregates of size N between 2 and 13 have been investigated. These crystallites exhibit well defined orientational order-disorder rotational transitions accompanied by a structural transition into a plastic crystallite phase. In addition, they exhibit melting and disassociation transitions. It is shown that the interpretation of experimental data, based upon dimer properties, depends crucially on these results. Equilibrium structures and orientations are also given.
Thermodynamic properties of compounds of carbon, hydrogen, nitrogen, oxygen, phosphorus, and sulfur
Thermodynamic properties for compounds of the elements carbon, hydrogen, nitrogen, oxygen, phosphorus, and sulfur
Effective pair potential obtained for quantum electron gas to determine thermodynamic properties over large temperature and density range
Thermodynamic properties of compounds of hydrogen, carbon, nitrogen, oxygen, phosphorus, and sulfur
Thermodynamic properties of carbon, hydrogen, oxygen, phosphorus, and sulfur compounds
Thermodynamic properties of carbon, hydrogen, nitrogen, oxygen, phosphorus, and sulfur compounds
Boltzmann distribution mechanics for digital calculations on equilibrium thermodynamic properties of air
Thermodynamic properties of various carbon- hydrogen-nitrogen-oxygen-phosphorus-sulfur compounds
Thermodynamic properties of amino acids plus furan and urea, and inorganic and organic compounds
Direct calculation and tables of specific heats and related thermodynamic properties of arbitrary gas mixtures - Mars atmosphere model
New, improved curve fits for the thermodynamic properties of equilibrium air have been developed. The curve fits are for pressure, speed of sound, temperature, entropy, enthalpy, density, and internal energy. These curve fits can be readily incorporated into new or existing computational fluid dynamics codes if real gas effects are desired. The curve fits are constructed from Grabau-type transition functions to model the thermodynamic surfaces in a piecewise manner. The accuracies and continuity of these curve fits are substantially improved over those of previous curve fits. These improvements are due to the incorporation of a small number of additional terms in the approximating polynomials and careful choices of the transition functions. The ranges of validity of the new curve fits are temperatures up to 25 000 K and densities from 10 to the -7 to 10 to the 3d power amagats.
New improved curve fits for the thermodynamic properties of equilibrium air were developed. The curve fits are for p = p(e,rho), a = a(e,rho), T = T(e,rho), s = s(e,rho), T = T(p,rho), h = h(p,rho), rho = rho(p,s), e = e(p,s) and a = a(p,s). These curve fits can be readily incorporated into new or existing Computational Fluid Dynamics (CFD) codes if real-gas effects are desired. The curve fits were constructed using Grabau-type transition functions to model the thermodynamic surfaces in a piecewise manner. The accuracies and continuity of these curve fits are substantially improved over those of previous curve fits appearing in NASA CR-2470. These improvements were due to the incorporation of a small number of additional terms in the approximating polynomials and careful choices of the transition functions. The ranges of validity of the new curve fits are temperatures up to 25,000 K and densities from 10 to the minus 7th to 100 amagats (rho/rho sub 0).
Gaseous and liquid neon thermodynamic properties with extrapolation to temperature and pressure ranges not available from experiment
An extremely compact object (ECO) is defined as a quantum object without horizon, whose radius is just a small distance s outside its Schwarzschild radius. We show that any ECO of mass M in d + 1 dimensions with s << (M/m p ) 2/(d-2)(d+1) lp must have (at leading order) the same thermodynamic properties—temperature, entropy and radiation rates—as the corresponding semiclassical black hole of mass M. An essential aspect of the argument involves showing that the Tolman–Oppenheimer–Volkoff equation has no consistent solution in the region just outside the ECO surface, unless this region is filled with radiation at the (appropriately blueshifted) Hawking temperature. In string theory it has been found that black hole microstates are fuzzballs—objects with no horizon—which are expected to have a radius that is only a little larger than the horizon radius. Thus the arguments of this paper provide a nice closure to the fuzzball paradigm: the absence of a horizon removes the information paradox, and the thermodynamic properties of the semiclassical hole are nonetheless recovered to an excellent approximation.
Remote sensing cross-beam cross correlation methods of determining spatially resolved average thermodynamic properties