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Kinetic theory of gases
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The temperature of an ideal monatomic gas is proportional to the average kinetic energy of its atoms. The size of helium atoms relative to their spacing is shown to scale under 1950 atmospheres of pressure. The atoms have a certain, average speed, slowed down here two trillion fold from room temperature.
The kinetic theory describes a gas as a large number of submicroscopic particles (atoms or molecules), all of which are in constant rapid motion that has randomness arising from their many collisions with each other and with the walls of the container.
Kinetic theory explains macroscopic properties of gases, such as pressure, temperature, viscosity, thermal conductivity, and volume, by considering their molecular composition and motion. The theory posits that gas pressure is due to the impacts, on the walls of a container, of molecules or atoms moving at different velocities.
Kinetic theory defines temperature in its own way, in contrast with the thermodynamic definition.[1]
Under a microscope, the molecules making up a liquid are too small to be visible, but the jittery motion of pollen grains or dust particles can be seen. Known as Brownian motion, it results directly from collisions between the grains or particles and liquid molecules. As analyzed by Albert Einstein in 1907, this experimental evidence for kinetic theory is generally seen as having confirmed the concrete material existence of atoms and molecules.
Contents
[hide]
1 Assumptions
2 Equilibrium properties
2.1 Pressure and kinetic energy
2.2 Temperature and kinetic energy
2.3 Collisions with container
2.4 Speed of molecules
3 Transport properties
3.1 Viscosity and kinetic momentum
4 History
5 See also
6 Notes
7 References
8 Further reading
9 External links
Assumptions[edit]
The theory for ideal gases makes the following assumptions:
The gas consists of very small particles known as molecules. This smallness of their size is such that the total volume of the individual gas molecules added up is negligible compared to the volume of the smallest open ball containing all the molecules. This is equivalent to stating that the average distance separating the gas particles is large compared to their size.
These particles have the same mass.
The number of molecules is so large that statistical treatment can be applied.
These molecules are in constant, random, and rapid motion.
The rapidly moving particles constantly collide among themselves and with the walls of the container. All these collisions are perfectly elastic. This means the molecules are considered to be perfectly spherical in shape and elastic in nature.
Except during collisions, the interactions among molecules are negligible. (That is, they exert no forces on one another.)
This implies:
1. Relativistic effects are negligible.
2. Quantum-mechanical effects are negligible. This means that the inter-particle distance is much larger than the thermal de Broglie wavelength and the molecules are treated as classical objects.
3. Because of the above two, their dynamics can be treated classically. This means that the equations of motion of the molecules are time-reversible.
The average kinetic energy of the gas particles depends only on the absolute temperature of the system. The kinetic theory has its own definition of temperature, not identical with the thermodynamic definition.
The elapsed time of a collision between a molecule and the container's wall is negligible when compared to the time between successive collisions.
Because they have mass, the gas molecules will be affected by gravity.
More modern developments relax these assumptions and are based on the Boltzmann equation. These can accurately describe the properties of dense gases, because they include the volume of the molecules. The necessary assumptions are the absence of quantum effects, molecular chaos and small gradients in bulk properties. Expansions to higher orders in the density are known as virial expansions.
An important book on kinetic theory is that by Chapman and Cowling.[1] An important approach to the subject is called Chapman–Enskog theory.[2] There have been many modern developments and there is an alternative approach developed by Grad based on moment expansions.[3] In the other limit, for extremely rarefied gases, the gradients in bulk properties are not small compared to the mean free paths. This is known as the Knudsen regime and expansions can be performed in the Knudsen number.
Equilibrium properties[edit]
Pressure and kinetic energy[edit]
In kinetic model of gases the pressure is equal to the force exerted by the atoms hitting and rebounding from a unit area of the gas container surface. Consider a gas of N molecules, each of mass m, enclosed in a cuboid of volume V = L3. When a gas molecule collides with the wall of the container perpendicular to the x axis and bounces off in the opposite direction with the same speed (an elastic collision), the change in momentum is given by:
Δ p = p i , x − p f , x = p i , x − ( − p i , x ) = 2 p i , x = 2 m v x , {\displaystyle \Delta p=p_{i,x}-p_{f,x}=p_{i,x}-(-p_{i,x})=2p_{i,x}=2mv_{x},}
where p is the momentum, i and f indicate initial and final momentum (before and after collision), x indicates that only the x direction is being considered, and v is the speed of the particle (which is the same before and after the collision).
The particle impacts one specific side wall once every
Δ t = 2 L v x , {\displaystyle \Delta t={\frac {2L}{v_{x}}},}
where L is the distance between opposite walls.
The force due to this particle is
F = Δ p Δ t = m v x 2 L . {\displaystyle F={\frac {\Delta p}{\Delta t}}={\frac {mv_{x}^{2}}{L}}.}
The total force on the wall is
F = N m v x 2 ¯ L , {\displaystyle F={\frac {Nm{\overline {v_{x}^{2}}}}{L}},}
where the bar denotes an average over the N particles.
Since the motion of the particles is random and there is no bias applied in any direction, the average squared speed in each direction is identical:
v x 2 ¯ = v y 2 ¯ = v z 2 ¯ . {\displaystyle {\overline {v_{x}^{2}}}={\overline {v_{y}^{2}}}={\overline {v_{z}^{2}}}.}
By Pythagorean theorem in three dimensions the total squared speed v is given by
v 2 ¯ = v x 2 ¯ + v y 2 ¯ + v z 2 ¯ , {\displaystyle {\overline {v^{2}}}={\overline {v_{x}^{2}}}+{\overline {v_{y}^{2}}}+{\overline {v_{z}^{2}}},}
v 2 ¯ = 3 v x 2 ¯ . {\displaystyle {\overline {v^{2}}}=3{\overline {v_{x}^{2}}}.}
Therefore:
v x 2 ¯ = v 2 ¯ 3 , {\displaystyle {\overline {v_{x}^{2}}}={\frac {\overline {v^{2}}}{3}},}
and the force can be written as:
F = N m v 2 ¯ 3 L . {\displaystyle F={\frac {Nm{\overline {v^{2}}}}{3L}}.}
This force is exerted on an area L2. Therefore, the pressure of the gas is
P = F L 2 = N m v 2 ¯ 3 V , {\displaystyle P={\frac {F}{L^{2}}}={\frac {Nm{\overline {v^{2}}}}{3V}},}
where V = L3 is the volume of the box.
In terms of the kinetic energy of the gas K:
P V = 2 3 × K . {\displaystyle PV={\frac {2}{3}}\times {K}.}
This is a first non-trivial result of the kinetic theory because it relates pressure, a macroscopic property, to the (translational) kinetic energy of the molecules N 1 2 m v 2 ¯ {\displaystyle N{\frac {1}{2}}m{\overline {v^{2}}}} , which is a microscopic property.
Temperature and kinetic energy[edit]
Rewriting the above result for the pressure as P V = N m v 2 ¯ 3 {\displaystyle PV={Nm{\overline {v^{2}}} \over 3}} , we may combine it with the ideal gas law
P V = N k B T , {\displaystyle \displaystyle PV=Nk_{B}T,}
(1)
where k B {\displaystyle \displaystyle k_{B}} is the Boltzmann constant and T {\displaystyle \displaystyle T} the absolute temperature defined by the ideal gas law, to obtain
k B T = m v 2 ¯ 3 {\displaystyle k_{B}T={m{\overline {v^{2}}} \over 3}} ,
which leads to simplified expression of the average kinetic energy per molecule,[4]
1 2 m v 2 ¯ = 3 2 k B T {\displaystyle \displaystyle {\frac {1}{2}}m{\overline {v^{2}}}={\frac {3}{2}}k_{B}T} .
The kinetic energy of the system is N times that of a molecule, namely K = 1 2 N m v 2 ¯ {\displaystyle K={\frac {1}{2}}Nm{\overline {v^{2}}}} . Then the temperature T {\displaystyle \displaystyle T} takes the form
T = m v 2 ¯ 3 k B {\displaystyle \displaystyle T={m{\overline {v^{2}}} \over 3k_{B}}}
(2)
which becomes
T = 2 3 K N k B . {\displaystyle \displaystyle T={\frac {2}{3}}{\frac {K}{Nk_{B}}}.}
(3)
Eq.(3) is one important result of the kinetic theory: The average molecular kinetic energy is proportional to the ideal gas law's absolute temperature. From Eq.(1) and Eq.(3), we have
P V = 2 3 K . {\displaystyle \displaystyle PV={\frac {2}{3}}K.}
(4)
Thus, the product of pressure and volume per mole is proportional to the average (translational) molecular kinetic energy.
Eq.(1) and Eq.(4) are called the "classical results", which could also be derived from statistical mechanics; for more details, see:[5]
Since there are 3 N {\displaystyle \displaystyle 3N} degrees of freedom in a monatomic-gas system with N {\displaystyle \displaystyle N} particles, the kinetic energy per degree of freedom per molecule is
K 3 N = k B T 2 {\displaystyle \displaystyle {\frac {K}{3N}}={\frac {k_{B}T}{2}}}
(5)
In the kinetic energy per degree of freedom, the constant of proportionality of temperature is 1/2 times Boltzmann constant. In addition to this, the temperature will decrease when the pressure drops to a certain point.[why?] This result is related to the equipartition theorem.
As noted in the article on heat capacity, diatomic gases should have 7 degrees of freedom, but the lighter gases act as if they have only 5.
Thus the kinetic energy per kelvin (monatomic ideal gas) is:
per mole: 12.47 J
per molecule: 20.7 yJ = 129 μeV.
At standard temperature (273.15 K), we get:
per mole: 3406 J
per molecule: 5.65 zJ = 35.2 meV.
Collisions with container[edit]
One can calculate the number of atomic or molecular collisions with a wall of a container per unit area per unit time.
Assuming an ideal gas, a derivation[6] results in an equation for total number of collisions per unit time per area:
N ∗ = 1 4 N V v avg = n 4 8 k B T π m . {\displaystyle N^{*}={\frac {1}{4}}{\frac {N}{V}}v_{\text{avg}}={\frac {n}{4}}{\sqrt {\frac {8k_{B}T}{\pi m}}}.}
This quantity is also known as the "impingement rate" in vacuum physics.
Speed of molecules[edit]
From the kinetic energy formula it can be shown that
v p = 2 ⋅ k B T m , {\displaystyle v_{\text{p}}={\sqrt {2\cdot {\frac {k_{\text{B}}T}{m}}}},}
v ¯ = 2 π v p = 8 π ⋅ k B T m , {\displaystyle {\bar {v}}={\frac {2}{\sqrt {\pi }}}v_{\text{p}}={\sqrt {{\frac {8}{\pi }}\cdot {\frac {k_{\text{B}}T}{m}}}},}
v rms = 3 2 v p = 3 ⋅ k B T m , {\displaystyle v_{\text{rms}}={\sqrt {\frac {3}{2}}}v_{\text{p}}={\sqrt {{3}\cdot {\frac {k_{\text{B}}T}{m}}}},}
where v is in m/s, T is in kelvins, and m is the mass of one molecule of gas. The most probable (or mode) speed v p {\displaystyle v_{\text{p}}} is 81.6% of the rms speed v rms {\displaystyle v_{\text{rms}}} , and the mean (arithmetic mean, or average) speed v ¯ {\displaystyle {\bar {v}}} is 92.1% of the rms speed (isotropic distribution of speeds).
See:
Average,
Root-mean-square speed
Arithmetic mean
Mean
Mode (statistics)
Transport properties[edit]
The kinetic theory of gases deals not only with gases in thermodynamic equilibrium, but also very importantly with gases not in thermodynamic equilibrium. This means considering what are known as "transport properties", such a viscosity and thermal conductivity.
Viscosity and kinetic momentum[edit]
In books on elementary kinetic theory[7] one can find results for dilute gas modeling that has widespread use. Derivation of the kinetic model for shear viscosity usually starts by considering a Couette flow where two parallel plates are separated by a gas layer. The upper plate is moving at a constant velocity to the right due to a force F. The lower plate is stationary, and an equal and opposite force must therefore be acting on it to keep it at rest. The molecules in the gas layer have a forward velocity component u {\displaystyle u} which increase uniformly with distance y {\displaystyle y} above the lower plate. The non-equilibrium flow is superimposed on a Maxwell-Boltzmann equilibrium distribution of molecular motions.
Let σ {\displaystyle \sigma } be the microscopic collision cross section of one molecule colliding with another. The macroscopic collision cross section of C ( = N / V e x t ) {\displaystyle C\left(=N/V_{ext}\right)} molecules per (extensive) volume is C σ {\displaystyle C\sigma } , and it is related to the mean free path l {\displaystyle l} by
l = 1 2 C σ {\displaystyle \quad l={\frac {1}{{\sqrt {2}}C\sigma }}}
Notice that the unit of the macroscopic collision cross section C σ {\displaystyle C\sigma } is reciprocal of length. The mean free path is the average distance traveled by a molecule, or a group of C {\displaystyle C} molecules per volume, before they make their first collision.
Let u 0 {\displaystyle u_{0}} be the forward velocity of the gas at the flat sliding surface SS. On the average, a molecule that crosses the sliding surface SS makes its last collision before crossing at a distance equal to two-thirds of the mean free path (i.e. 2 l / 3 {\displaystyle 2l/3} ) away from the surface. At this distance above and below the surface SS, the forward momentum of the molecule is respectively
p x ± = m ( u 0 ± 2 3 l d u d y ) {\displaystyle \quad p_{x}^{\pm }=m\left(u_{0}\pm {\frac {2}{3}}l{du \over dy}\right)}
where m is the molecular mass. The molecular flux Φ {\displaystyle \Phi } includes all molecules arriving at one side of an element of an imaginary horizontal surface SS within the gas layer. The incoming molecules are coming from all directions at the one side of the surface and with all speeds. This molecular flux (i.e. the number flux) is related to the average molecular speed v ¯ {\displaystyle {\bar {v}}} by
Φ = 1 4 v ¯ C {\displaystyle \quad \Phi ={\frac {1}{4}}{\bar {v}}C}
Notice that the forward velocity gradient d u / d y {\displaystyle du/dy} can be considered to be constant over a distance of mean free path. Next we multiply by the total flux to get the change of momentum per unit time and per unit area, that is carried by the molecules crossing from either above or below the surface area. This gives the equation
Φ p x ± = 1 4 v ¯ C ⋅ m ( u 0 ± 2 3 l d u d y ) {\displaystyle \quad \Phi p_{x}^{\pm }={\frac {1}{4}}{\bar {v}}C\cdot m\left(u_{0}\pm {\frac {2}{3}}l{du \over dy}\right)}
The net rate of momentum per unit area that is transported across the surface SS is thus
τ = Φ p x + − Φ p x − = 1 3 v ¯ C m ⋅ l d u d y {\displaystyle \quad \tau =\Phi p_{x}^{+}-\Phi p_{x}^{-}={\frac {1}{3}}{\bar {v}}Cm\cdot l{du \over dy}}
The defining equation for the (shear) viscosity η {\displaystyle \eta } of the gas is
F A = η d u d y {\displaystyle \quad {\frac {F}{A}}=\eta {du \over dy}}
Combining the above kinetic equation with defining equation for (shear) viscosity by τ = F / A {\displaystyle \tau =F/A} gives the equation for shear viscosity, which is usually denoted η 0 {\displaystyle \eta _{0}} when it is a dilute gas:
η 0 = 1 3 v ¯ C m l {\displaystyle \quad \eta _{0}={\frac {1}{3}}{\bar {v}}Cml}
Combining this equation with the equation for mean free path gives
η 0 = 1 3 2 m ⋅ v ¯ σ {\displaystyle \quad \eta _{0}={\frac {1}{3{\sqrt {2}}}}{\frac {m\cdot {\bar {v}}}{\sigma }}}
From statistical thermodynamics for gases we have equations relating average molecular speed to most likely speed and further to temperature. These statistical results gives the average (equilibrium) molecular speed as
v ¯ = 2 π v p = 2 2 π ⋅ k B T m {\displaystyle \quad {\bar {v}}={\frac {2}{\sqrt {\pi }}}v_{p}=2{\sqrt {{\frac {2}{\pi }}\cdot {\frac {k_{B}T}{m_{}}}}}}
where v p {\displaystyle v_{p}} is the most probable speed, k B {\displaystyle k_{B}} is the Boltzmann constant. We note that
k B ⋅ N A = R and M = m ⋅ N A {\displaystyle \quad k_{B}\cdot N_{A}=R\quad {\text{and}}\quad M=m\cdot N_{A}}
and insert the velocity in the viscosity equation above. This gives the well known equation for shear viscosity for dilute gases:
η 0 = 2 3 π ⋅ m k B T σ = 2 3 π ⋅ M R T σ ⋅ N A {\displaystyle \quad \eta _{0}={\frac {2}{3{\sqrt {\pi }}}}\cdot {\frac {\sqrt {mk_{B}T}}{\sigma }}={\frac {2}{3{\sqrt {\pi }}}}\cdot {\frac {\sqrt {MRT}}{\sigma \cdot N_{A}}}}
and M {\displaystyle M} is the molar mass. The equation above presupposes that the gas density is low (i.e. the pressure is low). This implies that the kinetic translational energy dominates over rotational and vibrational molecule energies. The viscosity equation further presupposes that there is only one type of gas molecules, and that the gas molecules are perfect elastic and hard core particles of spherical shape. This assumption of elastic, hard core spherical molecules, like billiard balls, implies that the microscopic collision cross section of one molecule can be estimated by
σ = π ( 2 r ) 2 = π d 2 {\displaystyle \quad \sigma =\pi \left(2r\right)^{2}=\pi d^{2}}
The radius r {\displaystyle r} is called collision cross section radius or kinetic radius, and the diameter d {\displaystyle d} is called collision cross section diameter or kinetic diameter of a molecule in a monomolecular gas. There are no simple general relation between the collision cross section and the hard core size of the (fairly spherical) molecule. The relation depends on shape of the potential energy of the molecule. For a real spherical molecule (i.e. a noble gas atom or a reasonably spherical molecule) the interaction potential is more like the Lennard-Jones potential or Morse potential which have a negative part that attracts the other molecule from distances longer than the hard core radius. The radius for zero Lennard-Jones potential is then appropriate to use as estimate for the kinetic radius.
Local nomenclature list:
A {\displaystyle A\ \ \ } : area of moving boundary in Couette flow experiment [m2]
C {\displaystyle C\ \ \ } : number concentration or number density [1/m3]
c {\displaystyle c\ \ \ \,} : molar concentration or molar density [mol/cm3]
d {\displaystyle d\ \ \ \,} : kinetic diameter in collision cross section [m]
F {\displaystyle F\ \ \ } : force that move a boundary in Couette flow experiment [N]
k B {\displaystyle k_{B}\ \,} : Boltzmann constant [JK−1]
l {\displaystyle l\ \ \ \ \ } : mean free path [m]
M {\displaystyle M\ \ } : molar mass [g/mol]
m {\displaystyle m\ \ \ } : molecular mass [Da]
N A {\displaystyle N_{A}\,} : Avogadro constant [mol−1]
P {\displaystyle P\ \ \ } : pressure [Pa or bar or atm]
P c {\displaystyle P_{c}\ \ } : critical pressure [Pa or bar or atm]
p x {\displaystyle p_{x}\ \ } : linear momentum in x-direction of a molecule [kgm/s]
R {\displaystyle R\ \ \ } : gas constant [JK−1mol−1]
r {\displaystyle r\ \ \ \,\,} : kinetic radius in collision cross section or hard core molecular radius [m]
T {\displaystyle T\ \ \,\,} : temperature [K]
T c {\displaystyle T_{c}\ \,\,} : critical temperature [K]
u {\displaystyle u\ \ \ \ } : macroscopic fluid velocity in x-direction [m/s]
u 0 {\displaystyle u_{0}\ \ } : macroscopic fluid velocity in x-direction of the fluid surface SS [m/s]
v ¯ {\displaystyle {\bar {v}}\ \ \ \ } : average molecular equilibrium speed [m/s]
v p {\displaystyle v_{p}\ \ \,} : most probable molecular equilibrium speed [m/s]
V {\displaystyle V\ \ \ } : molar volume [cm3/mol]
V c {\displaystyle V_{c}\ \ } : critical molar volume [cm3/mol]
V e x t {\displaystyle V_{ext}} : extensive fluid volume [m3]
y {\displaystyle y\ \ \ \ } : distance from non-moving boundary in direction normal to fluid flow [m]
η {\displaystyle \eta \ \ \ \ } : viscosity [Pas or μP or cP]
η 0 {\displaystyle \eta _{0}\ \,\,} : viscosity of dilute gas [Pas or μP or cP]
Φ {\displaystyle \Phi \ \ \,\,} : molecular flux across sliding surface SS [m−2s−1]
σ {\displaystyle \sigma \ \ \ \ } : collision cross section [m2]
τ {\displaystyle \tau \ \ \ \ } : shear stress [Nm−2]
K r {\displaystyle K_{r}\ } : dummy
History[edit]
In approximately 50 BCE, the Roman philosopher Lucretius proposed that apparently static macroscopic bodies were composed on a small scale of rapidly moving atoms all bouncing off each other.[8] This Epicurean atomistic point of view was rarely considered in the subsequent centuries, when Aristotlean ideas were dominant.
Hydrodynamica front cover
In 1738 Daniel Bernoulli published Hydrodynamica, which laid the basis for the kinetic theory of gases. In this work, Bernoulli posited the argument, still used to this day, that gases consist of great numbers of molecules moving in all directions, that their impact on a surface causes the gas pressure that we feel, and that what we experience as heat is simply the kinetic energy of their motion. The theory was not immediately accepted, in part because conservation of energy had not yet been established, and it was not obvious to physicists how the collisions between molecules could be perfectly elastic.[9]:36–37
Other pioneers of the kinetic theory (which were neglected by their contemporaries) were Mikhail Lomonosov (1747),[10] Georges-Louis Le Sage (ca. 1780, published 1818),[11] John Herapath (1816)[12] and John James Waterston (1843),[13] which connected their research with the development of mechanical explanations of gravitation. In 1856 August Krönig (probably after reading a paper of Waterston) created a simple gas-kinetic model, which only considered the translational motion of the particles.[14]
In 1857 Rudolf Clausius, according to his own words independently of Krönig, developed a similar, but much more sophisticated version of the theory which included translational and contrary to Krönig also rotational and vibrational molecular motions. In this same work he introduced the concept of mean free path of a particle. [15] In 1859, after reading a paper on the diffusion of molecules by Rudolf Clausius, Scottish physicist James Clerk Maxwell formulated the Maxwell distribution of molecular velocities, which gave the proportion of molecules having a certain velocity in a specific range.[16] This was the first-ever statistical law in physics.[17] Maxwell also gave the first mechanical argument that molecular collisions entail an equalization of temperatures and hence a tendency towards equilibrium.[18] In his 1873 thirteen page article 'Molecules', Maxwell states: "we are told that an 'atom' is a material point, invested and surrounded by 'potential forces' and that when 'flying molecules' strike against a solid body in constant succession it causes what is called pressure of air and other gases."[19] In 1871, Ludwig Boltzmann generalized Maxwell's achievement and formulated the Maxwell–Boltzmann distribution. Also the logarithmic connection between entropy and probability was first stated by him.
In the beginning of the twentieth century, however, atoms were considered by many physicists to be purely hypothetical constructs, rather than real objects. An important turning point was Albert Einstein's (1905)[20] and Marian Smoluchowski's (1906)[21] papers on Brownian motion, which succeeded in making certain accurate quantitative predictions based on the kinetic theory.
See also[edit]
Statistical mechanics
Thermodynamics
Kinetic theory
Particle statistics[show]
Spin-statistics theorem
Identical particles
Maxwell–Boltzmann
Bose–Einstein
Fermi–Dirac
Parastatistics
Anyonic Statistics
Braid Statistics
Thermodynamic ensembles[show]
NVE Microcanonical
NVT Canonical
µVT Grand canonical
NPH Isoenthalpic–isobaric
NPT Isothermal–isobaric
Models[show]
Debye
Einstein
Ising
Potts
Potentials[show]
Internal energy
Enthalpy
Helmholtz free energy
Gibbs free energy
Grand potential / Landau free energy
Scientists[show]
Maxwell
Boltzmann
Gibbs
Einstein
Ehrenfest
von Neumann
Tolman
Debye
Fermi
Bose
v
t
e
Bogoliubov-Born-Green-Kirkwood-Yvon hierarchy of equations
Boltzmann equation
Collision theory
Critical temperature
Gas laws
Heat
Interatomic potential
Magnetohydrodynamics
Maxwell–Boltzmann distribution
Mixmaster dynamics
Thermodynamics
Vlasov equation
Notes[edit]
^ Jump up to: a b Chapman, S., Cowling, T.G. (1939/1970).
Jump up ^ Kauzmann, W. (1966). Kinetic Theory of Gasses, W.A. Benjamin, New York, pp. 232–235.
Jump up ^ Grad 1949
Jump up ^ The average kinetic energy of a fluid is proportional to the root mean-square velocity, which always exceeds the mean velocity - Kinetic Molecular Theory
Jump up ^ Configuration integral (statistical mechanics) Archived 2012-04-28 at the Wayback Machine.
Jump up ^ Collisions With a Surface.
Jump up ^ Sears, F.W.; Salinger, G.L. (1975). "10". Thermodynamics, Kinetic Theory, and Statistical Thermodynamics (3 ed.). Reading, Massachusetts, USA: Addison-Wesley Publishing Company, Inc. pp. 286–291. ISBN 978-0201068948.
Jump up ^ Maxwell, J. C. (1867). "On the Dynamical Theory of Gases". Philosophical Transactions of the Royal Society of London. 157: 49. doi:10.1098/rstl.1867.0004.
Jump up ^ L.I Ponomarev; I.V Kurchatov (1 January 1993). The Quantum Dice. CRC Press. ISBN 978-0-7503-0251-7.
Jump up ^ Lomonosov 1758
Jump up ^ Le Sage 1780/1818
Jump up ^ Herapath 1816, 1821
Jump up ^ Waterston 1843
Jump up ^ Krönig 1856
Jump up ^ Clausius 1857
Jump up ^ See:
Maxwell, J.C. (1860) "Illustrations of the dynamical theory of gases. Part I. On the motions and collisions of perfectly elastic spheres," Philosophical Magazine, 4th series, 19 : 19–32.
Maxwell, J.C. (1860) "Illustrations of the dynamical theory of gases. Part II. On the process of diffusion of two or more kinds of moving particles among one another," Philosophical Magazine, 4th series, 20 : 21–37.
Jump up ^ Mahon, Basil (2003). The Man Who Changed Everything – the Life of James Clerk Maxwell. Hoboken, NJ: Wiley. ISBN 0-470-86171-1. OCLC 52358254.
Jump up ^ Gyenis, Balazs (2017). "Maxwell and the normal distribution: A colored story of probability, independence, and tendency towards equilibrium". Studies in History and Philosophy of Modern Physics. 57: 53–65. arXiv:1702.01411  . Bibcode:2017SHPMP..57...53G. doi:10.1016/j.shpsb.2017.01.001.
Jump up ^ Maxwell 1875
Jump up ^ Einstein 1905
Jump up ^ Smoluchowski 1906
References[edit]
Clausius, R. (1857), "Ueber die Art der Bewegung, welche wir Wärme nennen", Annalen der Physik, 176 (3): 353–379, Bibcode:1857AnP...176..353C, doi:10.1002/andp.18571760302
de Groot, S. R., W. A. van Leeuwen and Ch. G. van Weert (1980), Relativistic Kinetic Theory, North-Holland, Amsterdam.
Einstein, A. (1905), "Über die von der molekularkinetischen Theorie der Wärme geforderte Bewegung von in ruhenden Flüssigkeiten suspendierten Teilchen" (PDF), Annalen der Physik, 17 (8): 549–560, Bibcode:1905AnP...322..549E, doi:10.1002/andp.19053220806
Grad, Harold (1949), "On the Kinetic Theory of Rarefied Gases.", Communications on Pure and Applied Mathematics, 2 (4): 331–407, doi:10.1002/cpa.3160020403
Herapath, J. (1816), "On the physical properties of gases", Annals of Philosophy, Robert Baldwin: 56–60
Herapath, J. (1821), "On the Causes, Laws and Phenomena of Heat, Gases, Gravitation", Annals of Philosophy, Baldwin, Cradock, and Joy, 9: 273–293
Krönig, A. (1856), "Grundzüge einer Theorie der Gase", Annalen der Physik, 99 (10): 315–322, Bibcode:1856AnP...175..315K, doi:10.1002/andp.18561751008
Le Sage, G.-L. (1818), "Physique Mécanique des Georges-Louis Le Sage", in Prévost, Pierre, Deux Traites de Physique Mécanique, Geneva & Paris: J.J. Paschoud, pp. 1–186
Liboff, R. L. (1990), Kinetic Theory, Prentice-Hall, Englewood Cliffs, N. J.
Lomonosov, M. (1970) [1758], "On the Relation of the Amount of Material and Weight", in Henry M. Leicester, Mikhail Vasil'evich Lomonosov on the Corpuscular Theory, Cambridge: Harvard University Press, pp. 224–233
Mahon, Basil (2003), The Man Who Changed Everything – the Life of James Clerk Maxwell, Hoboken, New Jersey: Wiley, ISBN 0-470-86171-1
Maxwell, James Clerk (1873), "Molecules", Nature, 417 (6892): 903, Bibcode:2002Natur.417..903M, doi:10.1038/417903a, PMID 12087385, archived from the original (– Scholar search) on February 9, 2007
Smoluchowski, M. (1906), "Zur kinetischen Theorie der Brownschen Molekularbewegung und der Suspensionen", Annalen der Physik, 21 (14): 756–780, Bibcode:1906AnP...326..756V, doi:10.1002/andp.19063261405
Waterston, John James (1843), Thoughts on the Mental Functions (reprinted in his Papers, 3, 167, 183.)
Williams, M. M. R. (1971), Mathematical Methods in Particle Transport Theory, Butterworths, London.
Further reading[edit]
Sydney Chapman and T. G. Cowling (1939/1970). The Mathematical Theory of Non-uniform Gases: An Account of the Kinetic Theory of Viscosity, Thermal Conduction and Diffusion in Gases, (first edition 1939, second edition 1952), third edition 1970 prepared in co-operation with D. Burnett, Cambridge University Press, London.
J. O. Hirschfelder, C. F. Curtiss, and R. B. Bird (1964). Molecular Theory of Gases and Liquids, second edition (Wiley).
R. L. Liboff (2003). Kinetic Theory: Classical, Quantum, and Relativistic Descriptions, third edition (Springer).
B. Rahimi and H. Struchtrup, Macroscopic and kinetic modelling of rarefied polyatomic gases, Journal of Fluid Mechanics, 806, 437–505, 2016. DOI: https://dx.doi.org/10.1017/jfm.2016.604
External links[edit]
Early Theories of Gases
Thermodynamics - a chapter from an online textbook
Temperature and Pressure of an Ideal Gas: The Equation of State on Project PHYSNET.
Introduction to the kinetic molecular theory of gases, from The Upper Canada District School Board
Java animation illustrating the kinetic theory from University of Arkansas
Flowchart linking together kinetic theory concepts, from HyperPhysics
Interactive Java Applets allowing high school students to experiment and discover how various factors affect rates of chemical reactions.
https://www.youtube.com/watch?v=47bF13o8pb8&list=UUXrJjdDeqLgGjJbP1sMnH8A A demonstration apparatus for the thermal agitation in gases.
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values: \displaystyle    T   =   {m\overline{v^2}\over 3 k_B}

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values: \displaystyle    T   =   \frac   {2}   {3}   \frac   {K}   {N k_B}.

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   \displaystyle
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   \displaystyle
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