How Does External Pressure Affect Internal Pressure Variation in a Sphere?

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Discussion Overview

The discussion revolves around the effects of external pressure on the internal pressure variation of a sphere buried in an elastic medium. Participants explore theoretical scenarios involving different elastic properties of the medium and the sphere's walls, considering both rigid and flexible cases. The conversation includes mathematical reasoning and hypothetical situations to understand the relationship between internal and external pressures.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Jen introduces the problem of determining the internal pressure variation when energy is applied to a sphere in different external pressure conditions.
  • Some participants question the properties of the "elastic medium," particularly how it responds to displacement and whether it behaves like a perfect fluid.
  • There is a discussion about the flexibility of the sphere's walls and how this affects the internal pressure in response to external pressure changes.
  • One participant suggests that if the medium does not increase in pressure when the sphere expands, the internal pressure change would be zero.
  • Another participant argues that a perfectly rigid wall would maintain internal pressure regardless of external pressure changes, while flexible walls would allow internal pressure to approach external pressure.
  • Mathematical relationships are proposed, including the equation relating external pressures and volume changes, with some participants seeking references for derivation.
  • There is a hypothetical scenario involving a piston in a cylinder under water pressure, used to illustrate the concepts of force, work, and volume displacement.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of the elastic medium and the sphere's walls, leading to multiple competing models regarding how internal pressure varies with external pressure. The discussion remains unresolved with no consensus reached on the best approach or solution.

Contextual Notes

Participants highlight the importance of clarifying assumptions about the elasticity of the medium and the rigidity of the sphere's walls, which significantly influence the outcomes of the discussion. The mathematical relationships proposed depend on these assumptions and are not universally applicable without further specification.

Jenq
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TL;DR
pressure variations of a sphere subjected to different pressures
Hi

A sphere with radius r is buried in an elastic ideal medium at pressure P1.
Inside the sphere I use energy E to create a variation of pressure of dP.
What variation dPx I would measure if the sphere was buried in a medium at pressure P2 using the same energy E?
Is it possible to solve this problem?

Thank you

Jen
 
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This "elastic medium". How does it respond to displacement? i.e. how does it respond when a spherical volume within begins to expand? How elastic is it?

For instance, is it a perfect fluid which responds by moving away with no increase in pressure at all?
 
How flexible are the walls of the sphere?
If perfectly rigid, how much would the internal pressure be affected by changes in the external pressure?
 
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jbriggs444 said:
This "elastic medium". How does it respond to displacement? i.e. how does it respond when a spherical volume within begins to expand? How elastic is it?

For instance, is it a perfect fluid which responds by moving away with no increase in pressure at all?
Yes, I am looking for a solution in the simplest conditions, e.g. perfect elastic medium that doesn't increase in pressure if the sphere expands.
 
Lnewqban said:
How flexible are the walls of the sphere?
If perfectly rigid, how much would the internal pressure be affected by changes in the external pressure?
I don't know the answer, for a perfectly rigid wall is it possible to find a relationship between the 2 pressures in steady conditions?
 
Jenq said:
Yes, I am looking for a solution in the simplest conditions, e.g. perfect elastic medium that doesn't increase in pressure if the sphere expands.
You asked for a result as a change in pressure in a medium that deflects with no change in pressure. That's an easy answer: Zero.

If you wanted to know about deflection instead, that's easy as well. ##\Delta E = P \Delta V##. Solve for delta V.

Edit: If you want to work on deriving that formula above, we can help with that. A good starting point would be a piston arrangement rather than an expanding sphere.
 
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Jenq said:
I don't know the answer, for a perfectly rigid wall is it possible to find a relationship between the 2 pressures in steady conditions?
I believe that the original problem should have clarified that important detail.

Please, see:
https://en.m.wikipedia.org/wiki/Ideal_gas_law

A rigid wall or container would not allow any change in internal volume; therefore, if internal temperature does not change (because there is no thermal energy transfer through those walls), internal pressure must remain the same, no matter how much the medium pressure changes.

The opposite extreme would be walls that can be expanded much without offering much resistance or elastic force.
In that case, the internal pressure value would be very much close to the external one.
Think of a soap bubble, for example; its internal pressure must be equal to the atmospheric pressure surrounding it.

A rubber balloon would be an intermediate situation between those two extremes.
 
jbriggs444 said:
You asked for a result as a change in pressure in a medium that deflects with no change in pressure. That's an easy answer: Zero.

If you wanted to know about deflection instead, that's easy as well. ##\Delta E = P \Delta V##. Solve for delta V.

Edit: If you want to work on deriving that formula above, we can help with that. A good starting point would be a piston arrangement rather than an expanding sphere.
Ah sorry I misunderstood, I meant the pressure exerted by the external environment on the sphere does not change if the pressure / volume inside the sphere changes.

The equation is useful to me: so we can say that ## P_1 \Delta V_1 = \Delta E = P_2 \Delta V_2## where ##P_1## and ##P_2## are the external pressures, right? If so, yes I would like to read a reference on how to derive that equation.
Thanks
 
Lnewqban said:
I believe that the original problem should have clarified that important detail.

Please, see:
https://en.m.wikipedia.org/wiki/Ideal_gas_law

A rigid wall or container would not allow any change in internal volume; therefore, if internal temperature does not change (because there is no thermal energy transfer through those walls), internal pressure must remain the same, no matter how much the medium pressure changes.

The opposite extreme would be walls that can be expanded much without offering much resistance or elastic force.
In that case, the internal pressure value would be very much close to the external one.
Think of a soap bubble, for example; its internal pressure must be equal to the atmospheric pressure surrounding it.

A rubber balloon would be an intermediate situation between those two extremes.
I see, then I think the case should fall into an intermediate situation. Otherwise in a pure elastic case the sphere should inflate till the internal pressure balances the external one ## \Delta P_x = \Delta P + P_2 - P_1 ## ?

Thank you for the useful link.
 
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Jenq said:
Ah sorry I misunderstood, I meant the pressure exerted by the external environment on the sphere does not change if the pressure / volume inside the sphere changes.

The equation is useful to me: so we can say that ## P_1 \Delta V_1 = \Delta E = P_2 \Delta V_2## where ##P_1## and ##P_2## are the external pressures, right? If so, yes I would like to read a reference on how to derive that equation.
Instead of a sphere, assume that we have a cylinder under a pool of water. One end of the cylinder is closed. The other end is open to the water. There is a piston mounted in the cylinder. The piston is free to move within the cylinder. It makes a tight seal with the sides. Friction is negligible.

We remove the water behind the piston so that only vacuum remains. Obviously, the pool water is pushing on the piston. So we have to brace the piston, holding it stationary against the water pressure.

Now we use some energy, pushing the piston away from our brace on the vacuum side and out toward the open pool.

Let us call the pool pressure at the depth of the cylinder "P".
Let us say that the piston has cross-sectional area "A".
Let us say that we have used energy "E" to move the piston.

We ask: "much volume does the piston cover when we apply this energy E"?We can start with how much force there is on the piston. Force is equal to pressure times area.$$F=PA$$How much distance (##\Delta x##) has the piston covered? Work is equal to force times distance. So$$E=F\Delta x$$Solving for ##\Delta x## and substituting ##PA## for ##F##, we get:$$\Delta x = \frac{E}{PA}$$Multiply through by PA and we get:$$PA\Delta x = E$$How much volume (##\Delta V##) has the piston swept out? Well that is area times displacement -- ##A \Delta x##. So we get $$P \Delta V = E$$QED
 
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