Doubts about the formula for hydrostatic water pressure on a vertical surface

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Discussion Overview

The discussion revolves around the formula for hydrostatic pressure in fluids, specifically water, and its application to vertical surfaces. Participants explore the derivation of the formula P = ρgh and question its validity in scenarios involving vertical interfaces, such as dams.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant expresses confusion about applying the hydrostatic pressure formula to vertical surfaces, arguing that there is no water "resting" on such surfaces.
  • Another participant counters that the dam must be holding water, implying that the pressure still applies.
  • A different viewpoint explains that hydrostatic pressure is derived from the weight of the fluid column above a point, which is valid regardless of the surface orientation.
  • Concerns are raised about whether the derivation of the pressure formula is applicable to vertical surfaces, with some participants suggesting it only holds for inclined or horizontal surfaces.
  • Several participants emphasize that fluids exert pressure equally in all directions, which supports the application of the formula to vertical surfaces.
  • A later reply acknowledges the principle of Pascal's law, which states that pressure acts equally in all directions, resolving some confusion for one participant.
  • Another participant highlights a common misunderstanding about fluid pressure, referencing a demonstration that illustrates how water exerts pressure in all directions.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the applicability of the hydrostatic pressure formula to vertical surfaces. Some argue that the derivation is valid in all cases, while others maintain that it only applies to horizontal or inclined surfaces.

Contextual Notes

Participants discuss the assumptions underlying the hydrostatic pressure formula and the implications of fluid behavior, but do not resolve the mathematical or conceptual uncertainties raised regarding vertical surfaces.

ezadam
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Hey guys,

So I have just learned that the formula for a fluid's hydrostatic pressure (let's say water for the purpose of simplification) in terms of depth is:

P = ρ * g * h

Now I have been reading a bit on my textbook and I found out that the derivation of this formula is based on the assumption that for a given water column with volume V and height h resting on an area A on a given surface, the pressure is:

P = F/A = mg/A = (ρV)g/A = ρ(Ah)g/A = ρgh

Now I've also noticed that the same formula is used even when dealing with vertical contact surfaces, which I don't understand because when in that case (let's say in the case of a dam with a horizontal interface), there is no water directly "resting" on the surface and thus we cannot use the given formula.

So could you please tell me what I have missed in my reasoning and the misunderstandings (if any) that I have about the concept ? Thanks in advance.

(Please note that I am not denying the existence of hydrostatic pressure, I am just saying that its expression shouldn't be that of the conventional ρgh)
 
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You state:
Now I've also noticed that the same formula is used even when dealing with vertical contact surfaces, which I don't understand because when in that case (let's say in the case of a dam with a horizontal interface), there is no water directly "resting" on the surface and thus we cannot use the given formula.

I'm having trouble making sense of your statement above.

If the dam is not holding the water in the reservoir behind the dam, what is keeping the water contained?
 
In the case of hydrostatic pressure, the pressure must equal the weight of all fluid pushing down on a given point to satisfy Newton's laws. So basically, you have a column of fluid from the surface to any arbitrary depth, h. Let's say that this fluid column has horizontal dimensions dx_1 and dx_2. The weight of this column is therefore the density times the volume of the column, or \rho g h \;dx_1 \;dx_2. This is a force, and we are looking for a pressure, so we just divide it by the area of the base of the column dx_1 \;dx_2. That leaves you with:

P = \rho g h

Since dx_i are infinitesimal, the pressure from that equation represents the pressure at any point in the fluid of depth h.

Pressure is actually the force felt as a result of many fluid particles colliding with a surface, and therefore it acts in all directions equally. With that in mind, a vertical surface and a horizontal surface will feel the same force for a given depth, h.
 
SteamKing,

Sorry my bad. When I said
dam with a horizontal interface
, I actually meant "with a vertical interface". Here's an image of the kind of dam I am talking about. I thought that since the weight of the water (in red) is parrallel to the water-dam contact surface (in green), then the water has no effect on it and thus we cannot derive the aforementioned pressure formula (ρgh)

nege9g.gif


Boneh3ad,

You said that:

In the case of hydrostatic pressure, the pressure must equal the weight of all fluid pushing down on a given point to satisfy Newton's laws.

Well I think that in this case, there is no fluid weight pushing down on any point of the surface, correct me if I am wrong ? Thus I still don't think that the derivation is valid. In a nutshell, I believe that your derivation holds when having an inclined or horizontal surface, but not in the case of a vertical one.
 
The point is that water is a fluid- that is, it exerts the same force in all directions, not just downward.
 
ezadam said:
Well I think that in this case, there is no fluid weight pushing down on any point of the surface, correct me if I am wrong ? Thus I still don't think that the derivation is valid. In a nutshell, I believe that your derivation holds when having an inclined or horizontal surface, but not in the case of a vertical one.

HallsofIvy said:
The point is that water is a fluid- that is, it exerts the same force in all directions, not just downward.

This.

That is just how you find the pressure at any point. This includes points that butt up against vertical surfaces, and like I mentioned after that, the nature of a fluid means that the pressure acts in all directions, including horizontally onto the surface it butts up against regardless of the fact that there is no fluid "sitting" on it.
 
Thank you so much guys, I just re-read Pascal's law and confirmed to myself that pression actually acts equally in all directions. Problem solved !
 
This question has come up several times recently. I am amazed that the fact that fluid pressure acts in all direction equally seems to be so little known.
There is a lovely demonstration for 13 year old kids that consists of a piston in a long tube with a spherical bulb on the end. The bulb has small holes all over its surface. You draw water up into the cylinder / bulb from a bucket of water then you hold it all at arms length and squish it all out. Water squirts out very convincingly in ALL DIRECTIONS. It's not a quantitative experiment but my simple description of what happens will not be a surprise to anyone.

Also, why are people surprised about the pressure in a dam when they have all found that water emerges from a hosepipe - not only when it's pointed down but whatever direction it's pointed in - up, down and sideways. Wake up you chaps! You've seen the maths now think about the experience.
 

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