Jump to content
Toggle sidebar
The Portal Wiki
Search
Create account
Personal tools
Create account
Log in
Pages for logged out editors
learn more
Talk
Contributions
Navigation
Intro to The Portal
Knowledgebase
Geometric Unity
Economic Gauge Theory
All Podcast Episodes
All Content by Eric
Ericisms
Learn Math & Physics
Graph, Wall, Tome
Community
The Portal Group
The Portal Discords
The Portal Subreddit
The Portal Clips
Community Projects
Wiki Help
Getting Started
Wiki Usage FAQ
Tools
What links here
Related changes
Special pages
Page information
More
Recent changes
File List
Random page
Editing
Navier-Stokes equation
(section)
Page
Discussion
English
Read
Edit
View history
More
Read
Edit
View history
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
<div class="floatright" style="text-align: center"> [[File:Navier_stokes.png|center|class=shadow|300px]] </div> From Wikipedia, the free encyclopedia In physics, the Navier–Stokes equations (/nævˈjeɪ stoʊks/), named after Claude-Louis Navier and George Gabriel Stokes, describe the motion of viscous fluid substances. These balance equations arise from applying Isaac Newton's second law to fluid motion, together with the assumption that the stress in the fluid is the sum of a diffusing viscous term (proportional to the gradient of velocity) and a pressure term—hence describing viscous flow. The main difference between them and the simpler Euler equations for inviscid flow is that Navier–Stokes equations also factor in the Froude limit (no external field) and are not conservation equations, but rather a dissipative system, in the sense that they cannot be put into the quasilinear homogeneous form: <math> {\mathbf {y} _{t}+\mathbf {A} (\mathbf {y} )\mathbf {y} _{x}=0.}{\displaystyle \mathbf {y} _{t}+\mathbf {A} (\mathbf {y} )\mathbf {y} _{x}=0} </math> The Navier–Stokes equations are useful because they describe the physics of many phenomena of scientific and engineering interest. They may be used to model the weather, ocean currents, water flow in a pipe and air flow around a wing. The Navier–Stokes equations, in their full and simplified forms, help with the design of aircraft and cars, the study of blood flow, the design of power stations, the analysis of pollution, and many other things. Coupled with Maxwell's equations, they can be used to model and study magnetohydrodynamics. The Navier–Stokes equations are also of great interest in a purely mathematical sense. Despite their wide range of practical uses, it has not yet been proven whether solutions always exist in three dimensions and, if they do exist, whether they are smooth – i.e. they are infinitely differentiable at all points in the domain. These are called the Navier–Stokes existence and smoothness problems. The Clay Mathematics Institute has called this one of the seven most important open problems in mathematics and has offered a US$1 million prize for a solution or a counterexample.
Summary:
Please note that all contributions to The Portal Wiki may be edited, altered, or removed by other contributors. If you do not want your writing to be edited mercilessly, then do not submit it here.
You are also promising us that you wrote this yourself, or copied it from a public domain or similar free resource (see
The Portal:Copyrights
for details).
Do not submit copyrighted work without permission!
Cancel
Editing help
(opens in new window)