HTML5 Simulation of Ideal Gas Kinetic Theory by Using the 2-Dimensional Hard Sphere Collision Model

2019 ◽  
Vol 69 (1) ◽  
pp. 69-76
Author(s):  
Wonkun OH*
Keyword(s):  
Kinetic Theory ◽  
Hard Sphere ◽  
Ideal Gas ◽  
Collision Model ◽  
Gas Kinetic Theory

Gas Phase Spin Relaxation of ZX3Y Molecules in the Dipolar Approximation

1975 ◽  
Vol 53 (7) ◽  
pp. 723-738 ◽  
Author(s):  
B. C. Sanctuary ◽  
R. F. Snider
Keyword(s):  
Kinetic Theory ◽  
Gas Phase ◽  
Magnetic Relaxation ◽  
Dipolar Coupling ◽  
Point Group ◽  
Group Symmetry ◽  
Subsequent Paper ◽  
Point Group Symmetry ◽  
Proper Treatment ◽  
Gas Kinetic Theory

The gas kinetic theory of nuclear magnetic relaxation of a polyatomic gas, as formulated in the previous paper, is evaluated for ZX3Y molecules relaxing via a dipolar coupling Hamiltonian. Stress is given to a proper treatment of point group symmetry, here C3v, and the possibility of molecular inversion is included. The detailed formula for the spin traces is however restricted to X nuclei with spin 1/2. A subsequent paper uses these results to elucidate the structure of the high density dependence of T1 forCF3H.

Gas Kinetic Theory of Entropy

2018 ◽  
pp. 201-231
Author(s):  
Bahman Zohuri ◽  
Patrick McDaniel
Keyword(s):  
Kinetic Theory ◽  
Gas Kinetic Theory

Numerical Navier-Stokes Solutions from Gas Kinetic Theory

1994 ◽  
Vol 114 (1) ◽  
pp. 9-17 ◽  
Author(s):  
Kun Xu ◽  
Kevin H. Prendergast
Keyword(s):  
Kinetic Theory ◽  
Navier Stokes ◽  
Gas Kinetic Theory

A reactive collision model for use in kinetic theory

1978 ◽  
Vol 68 (2) ◽  
pp. 345-353 ◽  
Author(s):  
Nicolas Xystris ◽  
John S. Dahler
Keyword(s):  
Kinetic Theory ◽  
Collision Model ◽  
Reactive Collision

scholarly journals On the temperature variation of the specific heats of hydrogen and nitrogen

1930 ◽  
Vol 126 (801) ◽  
pp. 204-212 ◽  
Keyword(s):  
Kinetic Theory ◽  
Temperature Variation ◽  
Characteristic Equation ◽  
Constant Pressure ◽  
Ideal Gas ◽  
Constant Volume ◽  
Specific Heats

The energy of a gram molecule of an ideal gas can be calculated from the kinetic theory. From this, by the application of the Maxwell-Boltzmann hypothesis, the molecular specific heats at constant volume, S v , of ideal monatomic and diatomic gases are deduced to be 3R /2 and 5R/2 respectively at all temperatures. R is the gas constant per gram molecule = 1⋅985 gm. cal./° C. The corresponding molecular specific heats at constant pressure, S p , can be obtained by the addition of R. In the case of real gases, which obey some form of characteristic equation other than P. V = R. T, it can be shown from thermodynamical considera­tions that the value of S p depends upon the pressure, but as the term involving the pressure also includes the temperature, S p is not independent of the tempera­ture but it increases in value as the temperature is reduced. Assuming the characteristic equation proposed by Callendar, i. e. , v - b ­­= RT/ p - c (where b is the co-volume, c is the coaggregation volume which is a function of the temperature of the form c = c 0 (T 0 /T) n , n being dependent on the nature of the gas), it is easy to show from the relation (∂S p /∂ р ) T = -T(∂ 2 ν /∂Τ 2 ) р , hat S p = S p 0 + n (n + 1) cp /T; and, by combining this with S p – S v = T(∂ p /∂Τ) v (∂ v /∂Τ) p = R(1 + ncp /RT) 2 , the corresponding values of S v can be obtained.

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