Fluid Flow between parallel infinite plates

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SUMMARY

This discussion focuses on fluid flow between two parallel infinite plates, specifically analyzing the velocity profile of the fluid, denoted as u_1(z), under steady and laminar conditions. The top plate moves with a velocity U, while the bottom plate remains stationary, leading to the conclusion that u_1(surface) equals zero at the free surface. The Navier-Stokes equation is applicable for determining u_1(z) in both regions, with the flow between the plates characterized as plane Couette flow. The complexity increases above the top plate, where the fluid dynamics resemble Stokes' first problem, and the jump balance equations for mass, momentum, and energy become essential for understanding the fluid-fluid interface.

PREREQUISITES
  • Understanding of fluid mechanics principles
  • Familiarity with the Navier-Stokes equations
  • Knowledge of plane Couette flow dynamics
  • Acquaintance with interfacial transport phenomena as described in Slattery's "Interfacial Transport Phenomena"
NEXT STEPS
  • Study the derivation and application of the Navier-Stokes equations in laminar flow scenarios
  • Explore the characteristics and implications of plane Couette flow
  • Investigate Stokes' first problem and its relevance to fluid dynamics above moving surfaces
  • Review jump balance equations for mass, momentum, and energy at fluid-fluid interfaces
USEFUL FOR

Fluid mechanics students, researchers in fluid dynamics, and engineers working on applications involving laminar flow between surfaces will benefit from this discussion.

hawaiifiver
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Hello

I am trying to understand some fluid mechanics

I have two parallel infinite plates with fluid between the plates and some fluid above the plates.
The fluid above the plates has a free surface exposed to the atmosphere. And we can neglect body forces.

The fluid flow (steady and laminar) is two dimensional in both regions, and velocity doesn't depend on x and y: u = u_1 (z) i

What can i say about the value of u_1 (z) at the free surface. is u_1(surface) = 0 if the top plate is moving with a velocity U i. The bottomn plate is stationary.

Also how would you use the Navier Stokes quation to find u_1 (z) in both regions.
 
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Between the plates is straightforward: it's plane Couette flow.

The fluid above the top plate is significantly more complex: if it were unbounded, it would be similar to Stokes' first problem- except you have suppressed the time dependence that makes the solution finite.

At the fluid-fluid interface, it gets very complicated. There are so-called jump balance equations for mass, momentum, and energy which are quite horrendous and I'm not going to try and write them here. They can be found in Slattery's "Interfacial Transport Phenomena", and relate the motion of the fluid on either side of the dividing surface to the dynamics of the interface.
 

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