Fluid Mechanics, Depth, Pressure

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Discussion Overview

The discussion revolves around the derivation of fluid pressure at varying depths in fluid mechanics, particularly focusing on the role of pressure differences and the effects of gravity on fluid equilibrium. Participants explore the mathematical representation of forces acting on a fluid element and the implications of pressure variation with altitude.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about the term "dp" in the context of pressure differences, questioning its derivation and significance in the equilibrium of fluid elements.
  • Another participant suggests using p(y) to clarify that pressure varies with height, indicating that the downward force at height y+dy includes an additional term for dp.
  • There is a discussion about how pressure varies with altitude due to the weight of the fluid above, with some participants noting that neglecting gravity would lead to uniform pressure throughout the fluid.
  • Participants debate the equilibrium of the fluid slab, with some asserting that the forces acting on it must balance, while others express uncertainty about the implications of pressure at both the top and bottom surfaces.
  • One participant acknowledges a better understanding of the forces involved after considering the net force in relation to gravity, suggesting that the upward force represented by Adp is counterintuitive.
  • Buoyant force is introduced as a concept related to pressure differences, with one participant noting their limited prior knowledge on the topic.

Areas of Agreement / Disagreement

Participants generally agree that pressure varies with depth due to the weight of the fluid, but there is no consensus on the interpretation of certain aspects of the derivation and the implications of pressure differences. Some participants express confusion and seek clarification, indicating that the discussion remains unresolved in parts.

Contextual Notes

There are unresolved questions regarding the assumptions made about fluid equilibrium and the role of gravity in pressure calculations. The discussion highlights varying interpretations of the mathematical representation of forces acting on fluid elements.

Who May Find This Useful

This discussion may be useful for students and enthusiasts of fluid mechanics, particularly those grappling with the concepts of pressure variation, fluid equilibrium, and buoyancy.

mathsciguy
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I'm having a little problem with my book as I was reading about fluid mechanics. The book seems to have skipped a bit of some crucial part (at least for me) during the derivation for fluid pressure at certain depths (where the weight of the fluid is not neglected).

Here, I'll try to reconstruct the derivation and try to point out the parts where it confused me.

First suppose we have a fluid with definite volume where its density is the same throughout, hence it's uniform. Now, if we take an element fluid with thickness dy then and its top and bottom surfaces are the same, say A. Its volume is dV=A*dy, it's mass dm=(rho)*dV=(rho)*A*dy, and its weight w is dmg=(rho)*g*A*dy.

Where rho is the density of the fluid.

When the book gave an analysis of the forces on the y-component of that certain element fluid, the upward force is given by F(upward) = pA. I understand that part since there is pressure (p) pressing the fluid at its bottom area. Now, when the book gave the downward forces, it's given by F(downward) = (p+dp)*A and this confused me, where did the additional dp come from? There is the p that presses the upper area of the fluid but what about dp? Also the other downward force is the weight, but the fluid is in equilibrium, so:

(Sum)Fy = pA-(p+dp)*A-W=0 *The fact that there is force p*A upward and downward plus the weight is also non intuitive for me.*

So yeah, the biggest question for me is dp in the derivation, what is that?
 
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hi mathsciguy! :smile:

(have a rho: ρ :wink:)
mathsciguy said:
… When the book gave an analysis of the forces on the y-component of that certain element fluid, the upward force is given by F(upward) = pA. I understand that part since there is pressure (p) pressing the fluid at its bottom area. Now, when the book gave the downward forces, it's given by F(downward) = (p+dp)*A and this confused me, where did the additional dp come from? There is the p that presses the upper area of the fluid but what about dp? Also the other downward force is the weight, but the fluid is in equilibrium, so:

(Sum)Fy = pA-(p+dp)*A-W=0 *The fact that there is force p*A upward and downward plus the weight is also non intuitive for me.*

So yeah, the biggest question for me is dp in the derivation, what is that?

it's more intuitive if we write p(y) instead of just p, where y is height

then the force upward at height y is Ap(y),

and the force downward at height y+dy is Ap(y+dy), = A{p(y) + dp} (where dp = (dp/dy) dy)

so the total force downward (excluding gravity) is A{p(y) + dp} - Ap(y) = Adp​

(and dp will be negative because y is height, not depth :wink:)
 
Thanks, I thought no one would reply since my post was kinda messy.

So the pressure really is different at differing altitudes, but I thought that was caused by considering the force done by the gravity I.e. the weight. Since there is weight then it gives a downward pressure at the top surface (of course I know that if I think of it like that then the element fluid will not be in equilibrium, but I think that's another question).

I've thought of that, since from what I know, if we consider the case where there is negligible force done by the gravity then the pressure is the same throughout the volume of the fluid, it's the same even if we consider the pressure done by fluid onto a part of itself.

Edit: I think, my confusion is caused by not being sure of why pressure vary in altitude. Would it vary in altitude if we neglect the weight of the fluid?
 
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mathsciguy said:
So the pressure really is different at differing altitudes, but I thought that was caused by considering the force done by the gravity I.e. the weight. Since there is weight then it gives a downward pressure at the top surface

yes, that's correct …

pressure = force per area, and the only force downward is the weight of the fluid above :smile:
(of course I know that if I think of it like that then the element fluid will not be in equilibrium, but I think that's another question).

not following you … the slab of height dy is in equilibrium :confused:
I've thought of that, since from what I know, if we consider the case where there is negligible force done by the gravity then the pressure is the same throughout the volume of the fluid, it's the same even if we consider the pressure done by fluid onto a part of itself.

Edit: I think, my confusion is caused by not being sure of why pressure vary in altitude. Would it vary in altitude if we neglect the weight of the fluid?

no, eg air is a fluid, and its density is negligible (for most bodies, not for balloons etc), which is why we usually regard atmospheric pressure as the same throughout the lab, regardless of height :wink:
 
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tiny-tim said:
yes, that's correct …

pressure = force per area, and the only force downward is the weight of the fluid above :smile:not following you …*the slab of height dy is in equilibrium :confused:

Sorry, what actually goes through my mind is this:
Not considering dy, Fnet = Ap(y)-w-Ap(y) = ma *Well, because I thought at both top and bottom A there is that same pressure p, we just got an additional pressure done by w.

I kind of get it now though, if we solve for the net force on parallel to gravity we could see that Adp=-W, and this makes sense to me now.

Many thanks sir tiny-tim.
 
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tiny-tim said:
yes, that's correct …
not following you …*the slab of height dy is in equilibrium :confused:

Sorry, what actually goes through my mind is this:
Not considering dy, Fnet = Ap(y)-w-Ap(y) = ma *Well, because I thought at both top and bottom A there is that same pressure p, we just got an additional pressure done by w.

I kind of get it now though, if we solve for the net force on the y-axis we could see that Adp=-W, and this makes sense to me now. It's kind of not very intuitive to see that Adp is an upward force. (I might be wrong all together on this, I hope not)

Many thanks sir tiny-tim.
 
mathsciguy said:
It's kind of not very intuitive to see that Adp is an upward force.

it is! … there's more pressure underneath than on top, and that's the buoyant force that helps that slab of fluid to float! :biggrin:
 
tiny-tim said:
it is! … there's more pressure underneath than on top, and that's the buoyant force that helps that slab of fluid to float! :biggrin:

Thanks, I haven't read about buoyant force in depth yet, it's a good thing I've got some idea.
 
mathsciguy said:
Thanks, I haven't read about buoyant force in depth …

well, that's where to find it! :biggrin:
 

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