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Thermodynamic Systems01:06

Thermodynamic Systems

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A thermodynamic system is a set of objects whose thermodynamic properties are of interest. The system is considered to be embedded in its surroundings or the environment. The system and its environment can exchange heat and do work on each other through a boundary that separates them. However, the immediate surroundings of the system interact with it directly and therefore have a much stronger influence on its behavior and properties.
Consider an example of  tea boiling in a kettle. The...
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Third Law of Thermodynamics02:38

Third Law of Thermodynamics

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A pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K) may be described by a single microstate, as its purity, perfect crystallinity,and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.
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Entropy02:39

Entropy

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Salt particles that have dissolved in water never spontaneously come back together in solution to reform solid particles. Moreover, a gas that has expanded in a vacuum remains dispersed and never spontaneously reassembles. The unidirectional nature of these phenomena is the result of a thermodynamic state function called entropy (S). Entropy is the measure of the extent to which the energy is dispersed throughout a system, or in other words, it is proportional to the degree of disorder of a...
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Entropy01:18

Entropy

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The first law of thermodynamics is quantitatively formulated via an equation relating the internal energy of a system, the heat exchanged by it, and the work done on it. A quantitative formulation of the second law of thermodynamics leads to defining a state function, the entropy.
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Enthalpy02:59

Enthalpy

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Chemists ordinarily use a property known as enthalpy (H) to describe the thermodynamics of chemical and physical processes. Enthalpy is defined as the sum of a system’s internal energy (E) and the mathematical product of its pressure (P) and volume (V):
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Path Between Thermodynamics States01:21

Path Between Thermodynamics States

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Consider the two thermodynamic processes involving an ideal gas that are represented by paths AC and ABC in Figure 1:
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Cooling Rate Dependent Ellipsometry Measurements to Determine the Dynamics of Thin Glassy Films
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Theoretical Rationale for a Thermodynamic Glass State.

Isaac C Sanchez1, Sean P O'Keefe1

  • 1McKetta Department of Chemical Engineering, The University of Texas , Austin, Texas 78712, United States.

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|August 31, 2016
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Summary
This summary is machine-generated.

The quasichemical approximation for the square-well fluid model predicts a stable liquid state at low temperatures, avoiding the "entropy catastrophe" seen in other models. This force-stabilized liquid density becomes independent of temperature, forming glass states.

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Area of Science:

  • Thermodynamics
  • Statistical Mechanics
  • Materials Science

Background:

  • Mean-field models like van der Waals (VDW) fail to accurately describe liquid behavior at low temperatures.
  • VDW models predict unrealistic divergences in attractive forces as temperature decreases.
  • Understanding low-temperature liquid states is crucial for materials science and thermodynamics.

Purpose of the Study:

  • To investigate the behavior of the square-well (SW) fluid model at low temperatures using a quasichemical approximation (QCSW).
  • To determine if the QCSW model can predict a stable liquid state and avoid the theoretical "entropy catastrophe" at low temperatures.
  • To compare the QCSW model's predictions with those of mean-field VDW models.

Main Methods:

  • Solving the square-well (SW) fluid model using a chemical potential route.
  • Employing the quasichemical approximation (QCSW) for theoretical calculations.
  • Analyzing the behavior of liquid density and entropy as temperature decreases.

Main Results:

  • The QCSW model predicts a limiting liquid density at low temperatures, falling between the SW triple point density and the hard sphere transition density.
  • Liquid entropy approaches an asymptotic value, thus preventing the "entropy catastrophe".
  • Attractive force contributions in the QCSW model asymptote to a fixed value, unlike the 1/T divergence in VDW models.

Conclusions:

  • The QCSW model successfully predicts a stable, force-stabilized liquid state at low temperatures, identified as glass states.
  • Attractive forces saturate at high densities, leading to a temperature-independent liquid density and fixed thermodynamic properties.
  • The QCSW model offers a more accurate description of liquid behavior at low temperatures compared to VDW models.