• Study Resource
  • Explore
    • Arts & Humanities
    • Business
    • Engineering & Technology
    • Foreign Language
    • History
    • Math
    • Science
    • Social Science

    Top subcategories

    • Advanced Math
    • Algebra
    • Basic Math
    • Calculus
    • Geometry
    • Linear Algebra
    • Pre-Algebra
    • Pre-Calculus
    • Statistics And Probability
    • Trigonometry
    • other →

    Top subcategories

    • Astronomy
    • Astrophysics
    • Biology
    • Chemistry
    • Earth Science
    • Environmental Science
    • Health Science
    • Physics
    • other →

    Top subcategories

    • Anthropology
    • Law
    • Political Science
    • Psychology
    • Sociology
    • other →

    Top subcategories

    • Accounting
    • Economics
    • Finance
    • Management
    • other →

    Top subcategories

    • Aerospace Engineering
    • Bioengineering
    • Chemical Engineering
    • Civil Engineering
    • Computer Science
    • Electrical Engineering
    • Industrial Engineering
    • Mechanical Engineering
    • Web Design
    • other →

    Top subcategories

    • Architecture
    • Communications
    • English
    • Gender Studies
    • Music
    • Performing Arts
    • Philosophy
    • Religious Studies
    • Writing
    • other →

    Top subcategories

    • Ancient History
    • European History
    • US History
    • World History
    • other →

    Top subcategories

    • Croatian
    • Czech
    • Finnish
    • Greek
    • Hindi
    • Japanese
    • Korean
    • Persian
    • Swedish
    • Turkish
    • other →
 
Profile Documents Logout
Upload
Quantum Hall effect and the topological number in graphene
Quantum Hall effect and the topological number in graphene

GEEN1103
GEEN1103

... Name ...
Tunneling and the Vacuum Zero
Tunneling and the Vacuum Zero

Document
Document

SOLUTIONS for Homework #4
SOLUTIONS for Homework #4

View the Sample
View the Sample

11-3 - Ithaca Public Schools
11-3 - Ithaca Public Schools

901 bubblemotion10 05
901 bubblemotion10 05

discrete bose-einstein systems in a box with low adiabatic invariant
discrete bose-einstein systems in a box with low adiabatic invariant

Errata for the 2015-2016 School Handbook
Errata for the 2015-2016 School Handbook

Self-adjoint operators and solving the Schrödinger equation
Self-adjoint operators and solving the Schrödinger equation

Concepts of condensed matter physics Spring 2014 Exercise #5
Concepts of condensed matter physics Spring 2014 Exercise #5

ESI Bose-Einstein Condensation as a Quantum Phase Transition in an Optical Lattice
ESI Bose-Einstein Condensation as a Quantum Phase Transition in an Optical Lattice

5.2 The Wave Equation
5.2 The Wave Equation

... Eventually, I am going to have to face the challenge, and come up with some serious mathematical theory to support this claim. If particles have wave properties and can be described by a wave function, there must be a wave equation for particles. I’m going to set out to find it. But one last time, l ...
PPT File
PPT File

... When there is no initial correlation between the quantum system and stochastic process, we obtain the time-convolutionless (TCL) quantum master equation ...
Emergent Properties of Discretized Wave
Emergent Properties of Discretized Wave

... At this point, this paper becomes speculative. I do not know what happens in these models on the scale of fundamental particles, because it is not possible to do simulations at that scale. Thus, I describe what may happen based on properties of the models and existing physics. Such speculation may b ...
Quantum (Separation of Variables) - Physics | Oregon State University
Quantum (Separation of Variables) - Physics | Oregon State University

... mass has no effect. We can therefore ignore the center-of-mass motion and concentrate only on the relative motion. We have arrived at a conclusion in the quantum analysis of the twobody problem that is similar to our analysis of the classical problem (but for different reasons). We have again replac ...
Workshop Modern Numerical Methods in Quantum Mechanics
Workshop Modern Numerical Methods in Quantum Mechanics

On least action principles for discrete quantum scales
On least action principles for discrete quantum scales

Ohmic vs Markovian heat bath — two-page
Ohmic vs Markovian heat bath — two-page

Fluids - Teach Engineering
Fluids - Teach Engineering

Defense Presentation
Defense Presentation

... energy states and the probability that a given state will be occupied. The probability that a given occupied. The probability that a given energy state will be occupied is given by the distribution occupied is given by the distribution function, but if there are more available energy states in a mor ...
Lecture Notes
Lecture Notes

Spacetime structures of continuous
Spacetime structures of continuous

... next to the harmonic oscillator, the particle in a box provides much insight into the quantum world 共e.g. 关1兴兲. Recently, the problem of a quantum mechanical particle initially characterized by a Gaussian wave packet and moving in an infinite box has been reexamined 关2–4兴. Surprisingly, this simple ...
Calculating Friction Loss
Calculating Friction Loss

< 1 ... 27 28 29 30 31 32 33 34 35 ... 48 >

Lattice Boltzmann methods

Lattice Boltzmann methods (LBM) (or Thermal Lattice Boltzmann methods (TLBM)) is a class of computational fluid dynamics (CFD) methods for fluid simulation. Instead of solving the Navier–Stokes equations, the discrete Boltzmann equation is solved to simulate the flow of a Newtonian fluid with collision models such as Bhatnagar-Gross-Krook (BGK). By simulating streaming and collision processes across a limited number of particles, the intrinsic particle interactions evince a microcosm of viscous flow behavior applicable across the greater mass.
  • studyres.com © 2025
  • DMCA
  • Privacy
  • Terms
  • Report