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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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In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
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Equilibrium Conditions for a Particle01:23

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When an object is in equilibrium, it is either at rest or moving with a constant velocity. There are two types of equilibrium: static and dynamic. Static equilibrium occurs when an object is at rest, while dynamic equilibrium occurs when an object is moving with a constant velocity. In both cases, there must be a balance of forces acting on the object.
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The Uncertainty Principle04:08

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Werner Heisenberg considered the limits of how accurately one can measure properties of an electron or other microscopic particles. He determined that there is a fundamental limit to how accurately one can measure both a particle’s position and its momentum simultaneously. The more accurate the measurement of the momentum of a particle is known, the less accurate the position at that time is known and vice versa. This is what is now called the Heisenberg uncertainty principle. He...
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Principle of Linear Impulse and Momentum for a System of Particles01:21

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In the context of a system of particles moving relative to an inertial frame of reference, the equation of motion is a crucial tool for understanding the dynamics of the system. This equation, which accounts for external forces acting on each particle, plays a fundamental role in describing the system's behavior.
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The Bohr Model02:18

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Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as the...
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Related Experiment Video

Updated: Feb 18, 2026

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
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An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

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Quantum stochastic trajectories: the Smoluchowski-Bohm equation.

Francesco Avanzini1, Giorgio J Moro

  • 1Dipartimento di Scienze Chimiche, Università di Padova, via Marzolo 1, 35131 Padova, Italy. francesco.avanzini@unipd.it giorgio.moro@unipd.it.

Physical Chemistry Chemical Physics : PCCP
|November 29, 2017
PubMed
Summary

This study introduces a computationally efficient quantum method to model molecular motion in open quantum systems. The new stochastic approach accurately captures quantum dynamics, enabling the study of phenomena like vibrational relaxation.

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Area of Science:

  • Quantum mechanics
  • Chemical physics
  • Computational chemistry

Background:

  • Characterizing molecular motion in a quantum framework is computationally intensive.
  • Existing methods struggle with the exact quantum mechanical description of nuclear positions over time.
  • Quantum molecular trajectories are theoretically described by Bohm trajectories but are computationally demanding.

Purpose of the Study:

  • To develop a computationally feasible method for describing quantum molecular dynamics in open systems.
  • To accurately capture the quantum features of molecular motion.
  • To provide a self-consistent quantum mechanical approach for molecular dynamics.

Main Methods:

  • Derivation of a Smoluchowski-type stochastic equation from Schrödinger-Bohm dynamics.
  • Utilizing projection operator techniques.
  • Analysis of equilibrium distribution (wave function's squared modulus integrated over environment degrees of freedom).
  • Validation against deterministic dynamics for a model system of six interacting harmonic oscillators.

Main Results:

  • A stochastic equation accurately characterizes molecular motions in open quantum systems.
  • Quantum features of motion are revealed through the equilibrium distribution.
  • The method's accuracy is confirmed by comparison with deterministic dynamics.
  • The approach offers a self-consistent quantum mechanical representation of molecular dynamics.

Conclusions:

  • The derived stochastic equation provides an accurate and computationally efficient method for studying quantum molecular dynamics.
  • This approach enables the investigation of key phenomena such as vibrational relaxation, conformational transitions, and activated processes.
  • The method offers a significant advantage in computational cost for full quantum mechanical molecular dynamics simulations.