Fluids Bernoulli and a pressure field

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SUMMARY

The discussion centers on the application of linearized Bernoulli's equation to a cylindrical fluid shape, specifically addressing the pressure field described by the equation ##p = p_0 + \rho \partial_t \phi : \vec{v} = -\nabla \phi##. The static pressure, ##p_0##, is necessary to maintain the fluid's static interface shape, while the transient pressure component is questioned for its existence. The conversation highlights the equilibrium state of a cylindrical liquid volume and its response to disturbances, leading to resonance and deformation of its shape.

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  • Understanding of linearized Bernoulli's equation
  • Knowledge of fluid dynamics principles
  • Familiarity with pressure fields in fluid mechanics
  • Concept of resonance in fluid systems
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  • Study the derivation and applications of linearized Bernoulli's equation
  • Research pressure field analysis in cylindrical coordinates
  • Explore the effects of disturbances on fluid shapes and resonance
  • Examine the relationship between static and transient pressures in fluid dynamics
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Students and professionals in fluid mechanics, engineers working with fluid dynamics, and researchers studying pressure fields and resonance in liquid systems will benefit from this discussion.

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I have a text that writes a pressure balance for a cylindrical shape of fluid, where the linearized Bernoulli gives the pressure field ##p = p_0+\rho\partial_t \phi : \vec{v} = -\nabla \phi## where ##\vec{v}## is the velocity vector. ##p_0## is the static pressure required to maintain the fluid's static interface shape.

Evidently gravity and kinetic energy are neglected. My question is, how is it simply ##p## equates to both the transient and ##p_0## quantity? Wouldn't there have to be a transient quantity corresponding to ##p## (wherever it's located?)
 
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joshmccraney said:
p0 is the static pressure required to maintain the fluid's static interface shape.

Could you explain that to me please ?
 
Nidum said:
Could you explain that to me please ?
There is a volume of liquid shaped as a cylinder, and a wire runs streamwise, attaching tangentially to the volume of liquid. The surrounding media is a fluid with negligible density compared to the cylindrical liquid. In equilibrium the liquids shape will be pure cylindrical. Disturb the volume slightly and it will start to resonate and note always be cylindrical (the cross-sectional circles won't be circles, but have small waves). Given this, is my post #1 clear now?
 
joshmccraney said:
Given this, is my post #1 clear now?

Sorry but I still don't entirely understand what you are doing . I can see now what the general idea of the problem is but I can't link that to your equations or the related question .

I'll let this one go I think . Thank you anyway for replying .
 
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