Simplified derivation of viscosity equation

In summary, the conversation discusses the movement of a fluid between two plates at a distance d from each other in the z-direction, where the top plate is slid at a constant speed v_0 in the x-direction while the bottom plate remains still. This creates a velocity gradient v_x(z), with v_x(d) = v0 and v_x(0) = 0. The discussion then moves on to the number of particles per unit area that pass through a horizontal slab, with the assumption that the z-velocity does not change during collisions. The final part of the conversation addresses the number of particles that come from above or below the slab.
  • #1
gbertoli
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Homework Statement


Think of a fluid between two plates at a distance d from each other in the z-direction; then slide the top plate at a constant speed v_0 in the x-direction while holding the bottom plate still. The fluid pushes back, so you need to apply a force F in order to keep the plate moving at constant speed. Near the top plate, friction makes the fluid move with speed v0, whereas near the bottom plate the fluid is stationary. This causes a velocity gradient v_x(z), with v_x(d) = v0 and v_x(0) = 0.
Take a slab of gas at some value z. Assume all particles have the same magnitude of z-velocity, |v_z| (but have a gradient in their v_x velocity as explained above). Half move up and half move down. Also assume they all collide for the last time exactly λ distance (the mean free path) before passing through the slab and in the process acquire the x-velocity v_x(d − λ) if they collide below the slab and go above and v_x(d+λ) if they collide above the slab and go below. Their z-velocity does not change during this collision (Can you explain why this is reasonable assumption?).
Knowing that the density of particles in the fluid is ρ = N/V , give the number of particles (∆N) per unit area that pass through the horizontal slab from below in a period of time ∆t. Assume ∆t|v_z| ≫ λ. How many cross from above?

The Attempt at a Solution


The assumption that the z-velocity doesn't change is reasonable if we move the plate slowly enough.

The particles pass through an horizontal slab, so the result is proportional to the z-component of the velocity. Also, the number of particles passing must be proportional to the particle density. We thus get
\begin{equation*}
\text{\# of particles per unit time per unit area} =\dfrac{\Delta N}{A\Delta t}= \rho |v_z |
\end{equation*}
I'm just not sure on how to figure out how many come from above or below. Also, I am not supposed to use the Maxwell distribution.
 
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  • #2
No worries I found the solution. Silly me.
 

Related to Simplified derivation of viscosity equation

1. What is the viscosity equation?

The viscosity equation is a mathematical expression that describes the relationship between viscosity (a measure of a fluid's resistance to flow) and other physical properties such as temperature and pressure.

2. How is the viscosity equation derived?

The viscosity equation is derived from the Navier-Stokes equations, which describe the motion of fluids. The derivation involves simplifying the equations by assuming certain conditions, such as a constant temperature and pressure, and then solving for the viscosity term.

3. What are the assumptions made in the simplified derivation of the viscosity equation?

In the simplified derivation, it is assumed that the fluid is incompressible, the flow is steady and laminar, and there is no external force acting on the fluid. Additionally, the temperature and pressure are assumed to be constant.

4. What are the limitations of the simplified viscosity equation?

The simplified viscosity equation is only accurate for laminar flow and does not account for turbulence. It also assumes a constant temperature and pressure, which may not be true in all situations. Additionally, it is only applicable to Newtonian fluids (fluids with a constant viscosity at a given temperature and pressure).

5. How is the viscosity equation used in practical applications?

The viscosity equation is used in a variety of practical applications, including the design of pipelines and pumps, the production of paints and coatings, and the study of fluid flow in engineering and environmental systems. It is also used in the development of new materials, such as lubricants and polymers, and in the analysis of blood flow in the human body.

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