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Encyclopedia > Thermodynamic limit

In physics and physical chemistry, the thermodynamic limit is reached as the number of particles (atoms or molecules) in a system N approaches infinity — or in practical terms, one mole or Avogadro's number ≈ 6 x 1023. The thermodynamic behavior of a system is asymptotically approximated by the results of statistical mechanics as N → ∞, and calculations using the various ensembles converge. Theoretically, this concerns manipulating factorials arising from Boltzmann's formula for the entropy, S = k log W, by using Stirling's approximation, which is justified only when applied to large numbers. But it probably has an empirical basis as well. Ordinary thermodynamics may not apply to collections of only a few atoms or molecules. Physics (from the Greek, (phúsis), nature and (phusiké), knowledge of nature) is the science concerned with the discovery and understanding of the fundamental laws which govern matter, energy, space, and time. ... Physical Chemistry is the combined science of physics, chemistry, thermodynamics, and quantum mechanics which functions to provide molecular-level interpretations of observed macroscopic phenomena. ... Atomic redirects here. ... In chemistry, a molecule is an aggregate of two or more atoms in a definite arrangement held together by chemical bonds [1] [2] [3] [4] [5]. Chemical substances are not infinitely divisible into smaller fractions of the same substance: a molecule is generally considered the smallest particle of a pure... Avogadros number, also called Avogadros constant (NA), named after Amedeo Avogadro, is formally defined to be the number of carbon-12 atoms in 12 grams (0. ... Thermodynamics (from the Greek thermos meaning heat and dynamics meaning power) is a branch of physics that studies the effects of changes in temperature, pressure, and volume on physical systems at the macroscopic scale by analyzing the collective motion of their particles using statistics. ... Statistical mechanics is the application of probability theory, which includes mathematical tools for dealing with large populations, to the field of mechanics, which is concerned with the motion of particles or objects when subjected to a force. ... Statistical mechanics is the application of probability theory, which includes mathematical tools for dealing with large populations, to the field of mechanics, which is concerned with the motion of particles or objects when subjected to a force. ... The beginning of the sequence of factorials (sequence A000142 in OEIS) In mathematics, the factorial of a number n is the product of all positive integers less than or equal to n. ... Ludwig Eduard Boltzmann (Vienna, Austrian Empire, February 20, 1844 – Duino near Trieste, September 5, 1906) was an Austrian physicist famous for his founding contributions in the fields of statistical mechanics and statistical thermodynamics. ... Ice melting - classic example of entropy increasing[1] described in 1862 by Rudolf Clausius as an increase in the disgregation of the molecules of the body of ice. ... The relative difference between (ln x!) and (x ln x - x) approaches zero as x increases. ...


In some simple cases, and at thermodynamic equilibrium, the results can be shown to be a consequence of the additivity property of independent random variables; namely that the variance of the sum is equal to the sum of the variances of the independent variables. In these cases, the physics of such systems close to the thermodynamic limit is governed by the central limit theorem in probability. In thermodynamics, a thermodynamic system is said to be in thermodynamic equilibrium when it is in thermal equilibrium, mechanical equilibrium, and chemical equilibrium. ... A random variable is a mathematical function that maps outcomes of random experiments to numbers. ... In probability theory and statistics, the variance of a random variable (or somewhat more precisely, of a probability distribution) is a measure of its statistical dispersion, indicating how its possible values are spread around the expected value. ... A central limit theorem is any of a set of weak-convergence results in probability theory. ...


For systems of large numbers of particles, the genesis of macroscopic behavior from its microscopic origins fades from view. For example, the pressure exerted by a fluid (gas or liquid) is the collective result of collisions between rapidly moving molecules and the walls of a container, and fluctuates on a microscopic temporal and spatial scale. Yet the pressure does not change noticeably on an ordinary macroscopic scale because these variations average out. The use of water pressure - the Captain Cook Memorial Jet in Lake Burley Griffin, Canberra. ... A fluid is defined as a substance that continually deforms (flows) under an applied shear stress regardless of the magnitude of the applied stress. ... In physics, a fluctuation is a variation in an extensive or intensive quantity, such as energy, density or voltage, from its spatial or temporal average. ... A pocket watch, a device used to keep time There are two distinct views on the meaning of time. ... Spatial scale provides a shorthand form for discussing relative lengths, areas, distances and sizes. ...


Even at the thermodynamic limit, there are still small detectable fluctuations in physical quantities, but this has a negligible effect on most sensible properties of a system. However, microscopic spatial density fluctuations in a gas scatter light (which is why the sky is blue). These fluctuations become quite large near the critical point in a gas/liquid phase diagram. In electronics, shot noise and Johnson-Nyquist noise can be measured. In chemistry and condensed matter physics, a critical point specifies the conditions (temperature, pressure) at which the liquid state of the matter ceases to exist. ... In physical chemistry and materials science, a phase diagram is a type of graph used to show the equilibrium conditions between the thermodynamically-distinct phases. ... Shot noise is a type of noise that occurs when the finite number of particles that carry energy, such as electrons in an electronic circuit or photons in an optical device, gives rise to detectable statistical fluctuations in a measurement. ... Johnson-Nyquist noise, thermal noise, Johnson noise, or Nyquist noise) is the noise generated by the equilibrium fluctuations of the electric current inside an electrical conductor, which happens regardless of any applied voltage, due to the random thermal motion of the charge carriers (the electrons). ...


Certain quantum mechanical phenomena near the absolute zero T = 0 present anomalies; e.g., Bose-Einstein condensation, superconductivity and superfluidity. Fig. ... Absolute zero is the lowest possible temperature where nothing could be colder, and no heat energy remains in a substance. ... A Bose–Einstein condensate is a phase of matter formed by bosons cooled to temperatures very near to absolute zero (0 kelvins or -273. ... A magnet levitating above a high-temperature superconductor (with boiling liquid nitrogen underneath), demonstrating the Meissner effect. ... Helium II will creep along surfaces in order to find its own level - after a short while, the levels in the two containers will equalize. ...


It is at the thermodynamic limit that the additivity property of macroscopic extensive variables is obeyed. That is, the entropy of two systems or objects taken together (in addition to their energy and volume) is the sum of the two separate values. In physics and chemistry, an extensive quantity (also referred to as an extensive variable) is a physical quantity whose value is proportional to the size of the system it describes. ... Volume is how much space a thing has. ...


  Results from FactBites:
 
Ideal chain - Wikipedia, the free encyclopedia (1673 words)
The relevancy of the model is however limited, even at the macroscopic scale, by the fact that it does not consider any excluded volume for monomers (or, to speak in chemical terms, that it neglects steric effects).
The most general answer is that the effect of thermal fluctuations tends to bring a thermodynamic system toward a macroscopic state that corresponds to a maximum in the number of microscopic states (or micro-states) that are compatible with this macroscopic state.
Since the expression depends on the central limit theorem, it is only exact in the limit of polymers containing a large number of monomers (or thermodynamic limit).
  More results at FactBites »


 

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