Steady state in fluid mechanics

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SUMMARY

In fluid mechanics, a steady-state flow allows for the cancellation of the time-dependent acceleration term in the Navier-Stokes equation, specifically the term \(\frac{\partial \vec{V}}{\partial t}\). However, the convective acceleration, represented by the material derivative \(\frac{D\vec{V}}{Dt}\), is not necessarily zero even in steady-state conditions. This distinction is crucial as it highlights that while time-dependent changes in velocity are absent, spatial changes can still result in acceleration. The discussion clarifies common misconceptions regarding the treatment of acceleration terms in the context of steady-state flow.

PREREQUISITES
  • Understanding of Navier-Stokes equations
  • Familiarity with fluid dynamics concepts such as steady-state flow
  • Knowledge of material derivatives in vector calculus
  • Basic principles of acceleration in fluid mechanics
NEXT STEPS
  • Study the derivation and application of the Navier-Stokes equations in fluid dynamics
  • Learn about the concept of material derivatives and their significance in fluid mechanics
  • Explore examples of steady-state flow and its implications in real-world scenarios
  • Investigate the differences between total and partial derivatives in the context of fluid flow
USEFUL FOR

Students and professionals in fluid mechanics, engineers working with fluid systems, and researchers analyzing flow behavior in various applications will benefit from this discussion.

Nikitin
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Hey! When a stream is steady-state, you can cancel the acceleration term in navier-stokes equation, right?

so:

\rho \vec{a} = 0 = - \nabla P + \rho \vec{g} + \mu \nabla ^2 \vec{V}

But there are many terms in the total acceleration which are not dependent on time! The acceleration term in navier stokes can be broken down into https://scontent-b-ams.xx.fbcdn.net/hphotos-prn2/1379985_10201506247874738_1799136895_n.jpg: Why do the acceleration terms with regards to distance (dx, dy, dz) disappear also? This makes no sense to me.
 
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Your premiss is incorrect. the acceleration won't necessarily be zero for a steady state flow.
 
At 02:03 or so the professor says the flow is steady-state and removes the acceleration term.
 
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Yes the \frac{\partial \vec{V}}{\partial t} term will be zero on account of it is a time dependent quantity and is defined as zero in a steady-state flow. It is an acceleration term and it goes to zero, so in that sense you are right. But the larger "acceleration term" you are trying to zero out is the "convective acceleration" and is not necessarily zero.
 
Even for a steady state flow, an observer moving with the flow velocity along a streamline can be accelerating (Lagrangian frame of reference). His velocity vector is changing with time. The acceleration equation you wrote down (which is the so called Material Derivative of the velocity) determines his acceleration quantitatively.

Chet
 
Okay, but why did the professor in the video in post #3 just say "steady state" and zero-out the
\frac{d\vec{V}}{dt} term then? He said nothing about assuming the convective acceleration is zero..

I'm really confused about this... :(

EDIT: AND OOPS, I see I made a typing mistake in the picture in the OP. The velocity differentiated with regards to Z should be multiplied by w.
 
Because \frac{d\vec{V}}{dt} is not the same as \frac{D\vec{V}}{Dt}. For a steady state flow, all \frac{d}{dt} terms are zero, but not all \frac{D}{Dt} terms are necessarily zero.
 
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oh crap. I just noticed that the professor wrote the PARTIAL derivative of u with respect to time, NOT the total derivative, as his acceleration term. How careless of me.

When I watched it I thought the professor wrote up the complete navier-stokes equation, but apparently he zeroed all the convective acceleration terms.

Okay, thanks everybody.
 

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