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It is far more common for collisions to occur in two dimensions; that is, the initial velocity vectors are neither parallel nor antiparallel to each other. Let's see what complications arise from this. The first idea is that momentum is a vector. Like all vectors, it can be expressed as a sum of perpendicular components (usually, though not always, an x-component and a y-component, and a z-component if necessary). Thus, when the statement of conservation of momentum is written for a...
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An elastic collision is one that conserves both internal kinetic energy and momentum. Internal kinetic energy is the sum of the kinetic energies of the objects in a system. Truly elastic collisions can only be achieved with subatomic particles, such as electrons striking nuclei. Macroscopic collisions can be very nearly, but not quite, elastic, as some kinetic energy is always converted into other forms of energy such as heat transfer due to friction and sound. An example of a nearly...
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The moment-of-momentum equation is a critical tool for analyzing the torque produced by the rotating blades of a wind turbine. This equation is derived by applying Newton's second law to a fluid particle, which states that the rate of change of linear momentum is equal to the external force acting on the particle.
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Atomic Nuclei: Types of Nuclear Relaxation01:28

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Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
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Related Experiment Video

Updated: Jan 3, 2026

15N CPMG Relaxation Dispersion for the Investigation of Protein Conformational Dynamics on the &#181;s-ms Timescale
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Central-moment-based Galilean-invariant multiple-relaxation-time collision model.

Xiaowen Shan1

  • 1Shenzhen Key Laboratory of Complex Aerospace Flows, Department of Mechanics and Aerospace Engineering, Southern University of Science and Technology, Shenzhen, Guangdong 518055, China.

Physical Review. E
|November 28, 2019
PubMed
Summary

This study corrects non-Galilean-invariant thermal diffusivity in Boltzmann equation models. The new method ensures Galilean invariant viscosity and thermal diffusivity for accurate fluid simulations.

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Area of Science:

  • Computational fluid dynamics
  • Statistical physics
  • Numerical analysis

Background:

  • Previous multiple-relaxation-time Boltzmann equation collision models exhibited non-Galilean-invariant thermal diffusivity.
  • This limitation affected the accuracy of hydrodynamic simulations.

Purpose of the Study:

  • To systematically correct the non-Galilean-invariant thermal diffusivity in Boltzmann equation collision models.
  • To develop a method that yields Galilean invariant viscosity and thermal diffusivity.

Main Methods:

  • Chapman-Enskog expansion applied to a multiple-relaxation-time Boltzmann equation.
  • Separate relaxation of central moments of the distribution function.
  • Velocity-space discretization preserving moments up to the fourth order.
  • Transformation of central moments to the absolute reference frame for evaluation.

Main Results:

  • Achieved mutually independent and Galilean invariant viscosity and thermal diffusivity.
  • Preserved the efficiency and accuracy of the streaming-collision time-stepping algorithm.
  • Demonstrated excellent numerical stability in high-Reynolds-number simulations using the lattice Boltzmann model.

Conclusions:

  • The proposed method effectively corrects thermal diffusivity in Boltzmann equation models.
  • The approach ensures Galilean invariance, enhancing the reliability of fluid dynamics simulations.
  • The lattice Boltzmann model shows promise for high-Reynolds-number flow studies.