A general way of deriving the Navier-Stokes equations from the basic laws of physics
Now, we shall transform these statements into equation by accounting for each term,
(25.1)
(25.2)
(25.3)
is the body force per unit mass.
( 25.5)
We know that is the general form of mass conservation equation (popularly known as the continuity equation), valid for both compressible and incompressible flows.
(25.8)
From Stokes's hypothesis we get, (25.9)
Invoking above two relationships into Eq.( 25.6) we get
(25.10)
This is the most general form of Navier-Stokes equation.
Exact Solutions Of Navier-Stokes Equations
Consider a class of flow termed as parallel flow in which only one velocity term is nontrivial and all the fluid particles move in one direction only.
So, we obtain
(25.11)
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1. What are the Navier-Stokes equations? |
2. How are the Navier-Stokes equations derived? |
3. What are the applications of the Navier-Stokes equations in mechanical engineering? |
4. Are the Navier-Stokes equations solvable for all fluid flow problems? |
5. What are the limitations of the Navier-Stokes equations? |
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