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Follow-Up to "Pressure Profile"

I posted a problem called Pressure Profile a few days ago. When I wrote the problem, I assumed that when you push on a box without causing it to slide (there is friction), the normal reaction pressure varies linearly with the position along the box.

And sure enough, you can uniquely solve for a linear pressure profile which maintains the box in stasis. This is done by writing and solving two equations which describe the conditions for stasis (2 equations and 2 unknowns).

I then wondered what would happen if we assumed a quadratic pressure variation of the form \(P(x) = \alpha x^{2} + \beta x + \gamma\). Now there are three unknown parameters, but still only two equations. I've found that if you simply choose the \(\gamma\) parameter and solve for the other two, you can easily come up with a quadratic profile which has the following properties:

1) Satisfies the two equations for stasis
2) Results in positive upward pressure for all values of x between 0 and L

And there are presumably infinitely many such solutions, since I've already just casually found three quadratic profiles that have the above two properties. I suppose it would be possible to find solutions of even higher order as well (5th, 11th, 27th, etc.).

So my questions are these:

1) In the real world, would the pressure profile indeed be linear, as I originally assumed when posting the problem?

2) If so, how does nature know not to choose any higher-order variations in the pressure, since they appear to work, as far as I can tell?

3) Is there another constraint that forces a linear variation that I have simply not considered?


For reference, here's the derivation for the general quadratic pressure profile, of which a linear profile is a special case.

\[dA = W dx\] \[P(x) = \alpha x^{2} + \beta x + \gamma\] \[dF = P dA\] \[d\tau = Px dA\]

\[Force: \frac{Mg}{W} = \int_{0}^{L} (\alpha x^{2} + \beta x + \gamma) dx \\ \implies \frac{Mg}{W} = \alpha \frac{L^3}{3} + \beta \frac{L^2}{2} + \gamma L \]

\[Torque \, about \, (0,0): \frac{Mg}{W} \frac{L}{2} + \frac{F}{W} \frac{H}{2} = \int_{0}^{L} (\alpha x^{3} + \beta x^{2} + \gamma x) dx \\ \implies \frac{Mg}{W} \frac{L}{2} + \frac{F}{W} \frac{H}{2} = \alpha \frac{L^4}{4} + \beta \frac{L^3}{3} + \gamma \frac{L^2}{2} \]

By choosing the \(\gamma\) parameter and solving the two equations for \( \alpha\) and \( \beta\), we can generate numerous quadratic solutions. By setting \( \alpha\) to zero and solving for the other two, we can uniquely generate a linear profile. Here are three example profiles that seem to work (pressure is positive between 0 and L and the two equations for stasis are satisfied):

1) \( \alpha = 0,\beta = 7.5,\gamma = 42.5 \)

2) \( \alpha = 11.25,\beta = -15.0,\gamma = 50.0 \)

3) \( \alpha = -33.75,\beta = 75.0,\gamma = 20.0 \)

Note by Steven Chase
1 month, 2 weeks ago

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Well, what forces are on a molecule in the fluid, and in particular at the surface? Josh Silverman Staff · 1 month, 2 weeks ago

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@Josh Silverman Gravity acts at all points inside the box. An external force is applied at the left side of the box. There is an upward normal reaction from the surface upon which the box sits, which can be described in terms of a variable pressure. There is a horizontal friction force which keeps the box from sliding. And there should also be some internal horizontal forces within the box keeping the various differential box slices from moving horizontally. If there weren't, the friction forces would cause them to move. Steven Chase · 1 month, 2 weeks ago

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@Steven Chase I see, originally I assumed you were talking about a liquid in an accelerating box—my mistake.

Are you assuming that the box doesn't deform at all under the force? Josh Silverman Staff · 1 month ago

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@Josh Silverman Yes, I assumed perfect rigidity of the box. I have added an appendix with more information. Steven Chase · 1 month ago

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@Josh Silverman It would be great if you could add your calculation for one or two of the profiles to the note, so we can really get at this. Josh Silverman Staff · 1 month ago

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yes , i think so too and when i solved the problem i had to assume that too , but i say you should do like i suggest here @Steven Chase at a distance x consider a strip or a should say a cuboid of length dx and the normal reaction force on it would be responsible for the weight balancing and if we consider it a normal block , the force applied at \( \cfrac {H}{2} \) would vary linearly along it and when you balance torques you get the normal reaction and it is correct because here you get the real thing and you do not have o assume anything , what do you say @Steven Chase Shubham Dhull · 1 month, 2 weeks ago

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@Shubham Dhull Greetings. I'm not sure I followed that. What additional constraint do you think forces a linear profile? Steven Chase · 1 month, 2 weeks ago

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@Steven Chase the density of the cuboid is supposed to be linear ( i wrote a "normal block ") that's why i said the force applied varies linearly along the block ....if the density is some function of x , then it would not vary linearly , do you follow it now ? i would love if post a question on that when the density rises exponentially :) @Steven Chase Shubham Dhull · 1 month, 2 weeks ago

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@Shubham Dhull Ok, I think I see what you mean. Yeah, feel free to post a follow-up problem if you want. Steven Chase · 1 month, 2 weeks ago

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