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16-6 The Equation of Continuity
16-6 The Equation of Continuity

Stokes` law - schoolphysics
Stokes` law - schoolphysics

The Momentum Equation
The Momentum Equation

ENSC 283 Week # 10, Tutorial # 6
ENSC 283 Week # 10, Tutorial # 6

Lecture 23 - MSU Physics
Lecture 23 - MSU Physics

... that the flow induced pressure difference is quite a surprisingly large. The fact that it is negative indicates that the pressure is LOWER on the high velocity side of the wing. Airplane airfoils are designed to produce lift, so the high velocity side of the flow is on the upper side of the wind. Ra ...
Acoustic wave equation
Acoustic wave equation

... Wavelength of a sine wave, λ, can be measured between any two consecutive points with the same phase, such as between adjacent crests, or troughs, or adjacent zero crossings with the same direction of transit, as shown. ...
Scissors Mode
Scissors Mode

Velocity Profile u(x,y) x y
Velocity Profile u(x,y) x y

Vertical structure of the atmosphere
Vertical structure of the atmosphere

... where v ≡ u , v ,  , with ω ≡ dp/dt is the "vertical velocity" in p-coordinate. Note that ω > 0 implies downward motion of the fluid parcel. The coordinate transformation would rely on the hydrostatic relation. For example, ...
1-d examples
1-d examples

Wave Packets - Centro de Física Teórica
Wave Packets - Centro de Física Teórica

... particle. The experiment is 100 times repeated. The time starts counting everytime at the beginning of the experiment. One obtains the following result. The particle is never found for x < −4.5, or for x > 5.5, 3 times in the interval −4.5 < x < −3.5, 1 time in the interval −3.5 < x < −2.5, 7 times ...
Team 5 - HydroEurope
Team 5 - HydroEurope

Chapter 6: Momentum and Collisions
Chapter 6: Momentum and Collisions

Additional comments on Process modeling material
Additional comments on Process modeling material

Document
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Physics in Ultracold atoms
Physics in Ultracold atoms

... ( x1 , x2 )  ( x2 , x1 ), + for boson and - for fermion Therefore, for fermion we have ( x, x)  0, i.e. fermions like to be far away, but bosons do like to be close ! ...
lectures10-11.ppt - Projects at Harvard
lectures10-11.ppt - Projects at Harvard

... Explicit: Euler is unconditionally unstable Explicit: Leapfrog cures the problem, but small timesteps Implicit: Crank-Nicolson is unitary and allows large time-steps, but it may become expensive unless specialized linear algebra is used Matter of taste somehow… Fluid methods must handle the quantum ...
College of Engineering and Computer Science Mechanical
College of Engineering and Computer Science Mechanical

lecture 10
lecture 10

... Wavefunctions, probability density and energies are as shown in the figure. ...
Analysis of technological processes and equipment
Analysis of technological processes and equipment

Dynamics of Bose-Einstein Condensates in Trapped Atomic Gases
Dynamics of Bose-Einstein Condensates in Trapped Atomic Gases

Master Class 2002
Master Class 2002

... Quantum Mechanical Effect – Decay is random We have to measure many decays and take the average to determine a real lifetime (in fact we need to fit the data) Relativistic Effects are important: Need to take account time dilation etc. ...
Waves and the Schroedinger Equation
Waves and the Schroedinger Equation

Latest Lattice Results for Baryon Spectroscopy
Latest Lattice Results for Baryon Spectroscopy

EX917: Scattering resonances due to poles of the resolvent
EX917: Scattering resonances due to poles of the resolvent

< 1 ... 34 35 36 37 38 39 40 41 42 ... 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.
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