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The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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Maxwell's thermodynamic relations are very useful in solving problems in thermodynamics. Each of Maxwell's relations relates a partial differential between quantities that can be hard to measure experimentally to a partial differential between quantities that can be easily measured. These relations are a set of equations derivable from the symmetry of the second derivatives and the thermodynamic potentials.
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There are two ways to determine the amount of heat involved in a chemical change: measure it experimentally, or calculate it from other experimentally determined enthalpy changes. Some reactions are difficult, if not impossible, to investigate and make accurate measurements for experimentally. And even when a reaction is not hard to perform or measure, it is convenient to be able to determine the heat involved in a reaction without having to perform an experiment.
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The free energy change for a reaction that occurs under the standard conditions of 1 bar pressure and at 298 K is called the standard free energy change. Since free energy is a state function, its value depends only on the conditions of the initial and final states of the system. A convenient and common approach to the calculation of free energy changes for physical and chemical reactions is by use of widely available compilations of standard state thermodynamic data. One method involves the...
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Updated: Aug 20, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
05:39

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

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A Schmidt Decomposition Approach to Quantum Thermodynamics.

André Hernandes Alves Malavazi1, Frederico Brito1

  • 1Instituto de Física de São Carlos, Universidade de São Paulo, C.P. 369, São Carlos 13560-970, SP, Brazil.

Entropy (Basel, Switzerland)
|November 24, 2022
PubMed
Summary
This summary is machine-generated.

We present a new thermodynamic theory for quantum systems using Schmidt decomposition. This exact and symmetrical framework precisely describes energy in quantum systems, even under strong coupling.

Keywords:
open quantum systemsquantum thermodynamicsstrong coupling

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Area of Science:

  • Quantum physics
  • Thermodynamics
  • Quantum information science

Background:

  • A unified thermodynamic theory for general autonomous quantum systems is lacking.
  • Current approaches often rely on approximations or semi-classical regimes.
  • Fundamental questions in quantum thermodynamics remain unanswered.

Purpose of the Study:

  • To develop a novel, unifying formalism for quantum thermodynamics.
  • To describe the thermodynamics of arbitrary bipartite autonomous quantum systems.
  • To provide an exact and symmetrical framework beyond standard regimes.

Main Methods:

  • Utilizing the Schmidt decomposition.
  • Developing a formalism for bipartite quantum systems.
  • Identifying local effective operators.

Main Results:

  • A simple, exact, and symmetrical framework for quantum thermodynamics.
  • Accurate description of energetics, including strong coupling scenarios.
  • Straightforward identification of local effective operators for internal energies.

Conclusions:

  • The proposed formalism offers a general approach to quantum thermodynamics.
  • Local effective operators naturally satisfy energy additivity.
  • This work advances the understanding of thermodynamics in quantum systems.