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Entropy and the Second Law of Thermodynamics01:20

Entropy and the Second Law of Thermodynamics

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The second law of thermodynamics can be stated quantitatively using the concept of entropy. Entropy is the measure of disorder of the system.
The relation  between entropy and disorder can be illustrated with the example of the phase change of ice to water. In ice, the molecules are located at specific sites giving a solid state, whereas, in a liquid form, these molecules are much freer to move. The molecular arrangement has therefore become more randomized. Although the change in average...
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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.
When an ideal gas expands isothermally, the disorder in the gas increases. From the molecular perspective, the gas molecules have more volume to move around in.
Consider an infinitesimal step in the expansion, which...
2.7K
The Second Law of Thermodynamics01:14

The Second Law of Thermodynamics

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In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Scientists refer to the measure of randomness or disorder within a system as entropy. High entropy means high disorder and low energy. To better understand entropy, think of a student’s bedroom. If no energy or work were put into it, the room would quickly become messy. It would exist in a very disordered state, one of high entropy. Energy must be...
5.4K
Entropy Change in Reversible Processes01:10

Entropy Change in Reversible Processes

2.6K
In the Carnot engine, which achieves the maximum efficiency between two reservoirs of fixed temperatures, the total change in entropy is zero. The observation can be generalized by considering any reversible cyclic process consisting of many Carnot cycles. Thus, it can be stated that the total entropy change of any ideal reversible cycle is zero.
The statement can be further generalized to prove that entropy is a state function. Take a cyclic process between any two points on a p-V diagram.
2.6K
Second Law of Thermodynamics02:49

Second Law of Thermodynamics

24.0K
In the quest to identify a property that may reliably predict the spontaneity of a process, a promising candidate has been identified: entropy. Processes that involve an increase in entropy of the system (ΔS > 0) are very often spontaneous; however, examples to the contrary are plentiful. By expanding consideration of entropy changes to include the surroundings, a significant conclusion regarding the relation between this property and spontaneity may be reached. In thermodynamic...
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Third Law of Thermodynamics02:38

Third Law of Thermodynamics

19.0K
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.
19.0K

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Gradient Systems and Asymmetric Relaxations in View of Riemannian Geometry.

Entropy (Basel, Switzerland)·2026
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Related Experiment Video

Updated: Jul 21, 2025

Uncoupling Coriolis Force and Rotating Buoyancy Effects on Full-Field Heat Transfer Properties of a Rotating Channel
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Uncoupling Coriolis Force and Rotating Buoyancy Effects on Full-Field Heat Transfer Properties of a Rotating Channel

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Thermodynamic Entropy as a Noether Invariant from Contact Geometry.

Alessandro Bravetti1, Miguel Ángel García-Ariza1, Diego Tapias2

  • 1Instituto de Investigaciones en Matemáticas Aplicadas y en Sistemas, Universidad Nacional Autónoma de Mexico, A. P. 70543, Ciudad de Mexico 04510, Mexico.

Entropy (Basel, Switzerland)
|July 29, 2023
PubMed
Summary

Researchers linked thermodynamic entropy to time-symmetry using Noether's theorem in Hamiltonian systems. For systems at equilibrium, this implies conserved total entropy, offering a geometric perspective on thermodynamics.

Keywords:
Hamiltonian systemsNoether’s theoremcontact geometryentropythermostatted systems

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Area of Science:

  • Thermodynamics
  • Geometric Mechanics
  • Mathematical Physics

Background:

  • Noether's theorem is fundamental in physics, connecting symmetries to conserved quantities.
  • Thermodynamic entropy is a key concept in understanding heat, work, and energy dispersal.
  • Contact Hamiltonian systems provide a framework for describing dissipative and conservative dynamics.

Purpose of the Study:

  • To establish a connection between thermodynamic entropy and Noether invariants in contact Hamiltonian systems.
  • To explore the implications of time-translational symmetry for entropy conservation.
  • To offer a geometric interpretation of thermodynamic entropy.

Main Methods:

  • Application of a specific formulation of Noether's theorem tailored for contact Hamiltonian systems.
  • Derivation of a mathematical relationship between thermodynamic entropy and the Noether invariant linked to time-translation symmetry.
  • Analysis of the specific case of thermostatted systems at thermodynamic equilibrium.

Main Results:

  • A direct relation is derived between thermodynamic entropy and the Noether invariant associated with time-translational symmetry.
  • For thermostatted systems in equilibrium, the total entropy of the system and its reservoir is shown to be conserved.
  • The findings provide a novel geometric perspective on the nature of thermodynamic entropy.

Conclusions:

  • The study successfully links symmetries, via Noether's theorem, to thermodynamic concepts like entropy.
  • Conservation of total entropy in equilibrium systems is demonstrated as a consequence of time-translational symmetry.
  • The geometric viewpoint enhances the fundamental understanding of thermodynamic entropy in physical systems.