Derivation of Hydrostatic Equations Fluids

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Discussion Overview

The discussion revolves around the derivation of hydrostatic equations in fluid mechanics, specifically focusing on understanding the forces acting on fluid particles in different directions (x, y, z). Participants explore the implications of body forces, particularly gravity, and how they relate to pressure gradients in various coordinate directions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant expresses difficulty in deriving hydrostatic equations with respect to x and z, noting confusion about the forces acting on fluid particles.
  • Another participant provides a vector equation for force per unit volume, indicating that pressure gradients and gravitational forces must balance for equilibrium.
  • Some participants clarify that the z-component of the force includes gravity, while the x and y components do not typically include body forces.
  • There is a discussion about the possibility of other forces, such as electromagnetic forces, being considered in the y-direction, although some participants assert that gravity is the primary force in hydrostatics.
  • One participant acknowledges the professor's loose terminology regarding body forces, suggesting that the presence of forces other than gravity could be implied but not explicitly stated.

Areas of Agreement / Disagreement

Participants generally agree that gravity is the primary body force in hydrostatics, particularly in the z-direction. However, there is disagreement regarding the presence of body forces in the y-direction, with some suggesting the possibility of other forces while others assert that typically only gravity is considered.

Contextual Notes

Participants note that the discussion may be complicated by the professor's vague explanations and the potential for misunderstanding regarding the inclusion of body forces in different directions. The exact nature of forces acting in the y-direction remains unclear.

jdawg
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Homework Statement


I'm having a little trouble understanding how to derive the hydrostatic equations for fluid mechanics!
My professor showed the derivation with respect to y in class, and it kind of made sense to me. Now I'm trying to see if I can derive the equation with respect to z and x.

I think part of my issue is that I don't fully understand the forces that are acting on the fluid particle. I know there are two surface forces and one body force for the y derivation. My professor mentioned that there is only a body force for the y and z directions, but didn't mention x. He said the body force in this case is gravity, which I understand why this force would be on the particle in the z direction, but why the y direction or x direction? How is gravity affecting the particle from the y direction or x direction?

Maybe the body force acting in the y direction isn't gravity? If its not what could it be and why is there no body force in the x direction?

I'm not sure if I drew the forces correctly in the figure 2 for the z direction. I'm also not sure about how to draw the forces for the x direction, would that case just be two surface forces in the x direction? One coming from the front of the box towards the particle and the other coming from the back of the box towards the particle?The summation of forces part I understand no problem. If y'all could help me figure out how to get to that point I think I'll be good!

From picture I attached:
SF1 = (p-(∂p/∂y)(dy/2))dxdz
SF2 = (p+(∂p/∂y)(dy/2))dxdz

SF3 = (p-(∂p/∂z)(dz/2))dxdy
SF4 = (p-(∂p/∂z)(dz/2))dxdy
BodyForceInZ = (ρdxdydz)bf-z

I hope my picture isn't too confusing, thanks for any help!
 

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This one is most easily written with one vector equation which you basically have derived above: The force per unit volume from pressure gradients is ## f_v=-\nabla P ##. The gravitational force per unit volume ## f_g=-\delta g \hat{z} ## (using upward as positive z.) In order to have equilibrium the net forces must be zero: ## -\nabla P- \delta g \hat{z} =0 ##. The ## -\nabla P ## is in general a vector with 3 components, thereby the x, y, and z equations.
 
That is much simpler! I think I'm expected to be able to derive each equation for x, y, and z individually though.
 
jdawg said:
That is much simpler! I think I'm expected to be able to derive each equation for x, y, and z individually though.
## -\nabla P=-[\frac{\partial P}{\partial x}\hat{x}+\frac{\partial P}{\partial y}\hat{y}+\frac{\partial P}{\partial z}\hat{z}] ##. The rest is simple. You have one equation for each vector component. The z-component is the only one that has any gravity in it.
 
According to the equations you presented, there is no body force component in the y direction.
 
Getting the equations isn't the part I'm struggling with, I'm trying to understand what forces are acting on the particle.
I didn't think it made sense for there to be a gravitational force in the x and y directions, but what is the body force if its not gravity?

Sorry I didn't include the body force in the written part, it drew it in the picture attached.
 
Chestermiller said:
According to the equations you presented, there is no body force component in the y direction.
Yes, the OP doesn't seem real clear on this. Is their professor considering the possibility of another force, e.g. an electromagnetic force of some kind in the y-direction? Normally, in an introduction to hydrostatics, gravity is the only force to consider besides pressure gradient forces.
 
There are no electromagnetic forces present, just gravity.
 
jdawg said:
There are no electromagnetic forces present, just gravity.
Then you normally don't get a body force in the y-direction.
 
  • #10
I'm not sure if they'll help, but here's a scan of my notes. Hopefully it isn't so light you can't read them.
 

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  • #11
jdawg said:
I'm not sure if they'll help, but here's a scan of my notes. Hopefully it isn't so light you can't read them.
I think the professor was talking very loosely. He seemed to be suggesting (from the notes) that you can have a body force in the y-direction, (or any direction for that matter). He didn't say so (at least your notes don't show it), but when other forces besides gravity are introduced in this kind of thing, it is oftentimes some type of electromagnetic force.
 
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  • #12
Ohh ok, I think that cleared up a lot of confusion. I wish he would've explained that a little better. I was going crazy trying to figure out how gravity was affecting the particle from the y direction. Thanks for y'alls help!
 
  • #13
Charles Link said:
Yes, the OP doesn't seem real clear on this. Is their professor considering the possibility of another force, e.g. an electromagnetic force of some kind in the y-direction? Normally, in an introduction to hydrostatics, gravity is the only force to consider besides pressure gradient forces.
I agree. In any event, the professor seems to be allowing for the possibility of a body force other than gravity.
 
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