Millennium Problem: Navier-Stokes existence and smoothness
Navier-Stokes equations are about motion of fluids.
Example of fluids being air and water. Mathematicians and physicists believe that an explanation
for both the breeze and the turbulence of fluids can be found through an
understanding of solutions to the Navier-Stokes equations. A fluid is something that you can assume to be a
continuum- i.e. not made of discrete particles. To this end, we can already see that the Navier-stokes
equations must be approximations, because fluids are made of atoms!
The Navier-Stokes equation has one final step which is to write down the form of the viscous force.
So we can see that just by applying Newton’s 2nd law to a small chunk of a fluid, we have derived:
This really is the incompressible Navier-Stokes equation!
Reference
The Navier-Stokes
equations are, in essence, just Newton’s
2nd law written in a form that is applicable to continuum bodies,
rather than discrete objects.
We know that Newton’s second law as F=ma, which can be written as
Where v is the
velocity. If we are dealing with a fluid, we don’t care about mass, we care
about density- which for now we assume is constant-i.e., the fluid is
incompressible.
Therefore, just by taking
the continuum form of Newton’s Second Law, we get:
Where f is the “body
force” – the infinitesimal force on an infinitesimal chunk of the fluid.
Since the velocity of
the fluid is both a function of space
and of time – we have:
We note that dx/dt are
just components of the velocity, and hence we can put this into a vector
notation:
Which means:
So now we need to think
about what these forces could be.
There are two types of
forces that can act on a fluid:
- Internal forces, due to interactions between the components
- External forces such as gravity
There are two major
internal forces that we need to consider: pressure forces, and the viscosity.
If we write this out,
we have:
f=fviscous +
fext - ∇P
Where P is the internal
pressure, and ∇ is just a vector derivative.
Substituting we get
The Navier-Stokes equation has one final step which is to write down the form of the viscous force.
The viscous force is the internal friction of all the particles rubbing up against each other, and takes the form:
So we can see that just by applying Newton’s 2nd law to a small chunk of a fluid, we have derived:
This really is the incompressible Navier-Stokes equation!
So that’s what it is,
in relatively simple terms: it is just “force is the product of mass times
acceleration” adjusted for pressure and viscosity.
The mathematics behind
this, however, is where things get interesting and challenging.
This is an incredibly hard equation to solve. We can solve it exactly for certain specific cases, and you can
make approximations to make it easier to study. It’s so difficult that
it has not even been proved that solutions always exist.
The prize problem can be
broken into two parts. The first focuses on the existence of solutions to the
equation. The second focuses on whether these solutions are bounded (remain
finite). If you are able to show that you will win $1,000,000.
Reference
http://www.claymath.org/sites/default/files/navierstokes.pdf
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