Balloon inflated by external vacuum: why won't it burst?

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    Balloon Vacuum
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Discussion Overview

The discussion revolves around the phenomenon of a balloon not bursting when inflated in a vacuum environment, exploring the underlying physics of pressure differentials, tensile strength, and material properties. Participants examine various theoretical and practical aspects related to this scenario.

Discussion Character

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

Main Points Raised

  • Some participants suggest that the differential pressure between the inside and outside of the balloon is crucial, similar to a conventionally inflated balloon.
  • Others propose that the pressure difference may not be sufficient to exceed the tensile strength of the balloon material.
  • One participant questions whether the inflated surface area of the balloon correlates with the pressure differential, noting that increasing surface area could coincide with a decreasing pressure differential.
  • Another participant introduces the Young-Laplace equation to describe the pressure differential in relation to curvature and surface tension, emphasizing the importance of curvature and tensile strength.
  • Some participants express skepticism about the relevance of the vacuum setup, suggesting it may mislead the understanding of balloon behavior.
  • One participant shares an anecdote about using a "funny balloon" (condom) in a demonstration, noting it filled the volume without bursting until constrained.
  • Another participant discusses the implications of Boyle's Law in relation to pressure differences and the behavior of the balloon under varying conditions.

Areas of Agreement / Disagreement

Participants do not reach a consensus, as multiple competing views remain regarding the factors influencing the balloon's behavior in a vacuum. There is ongoing debate about the significance of pressure differentials, material properties, and the effects of curvature.

Contextual Notes

Some limitations include assumptions about the balloon's material properties, the definitions of pressure differentials, and the conditions under which the balloon is inflated. The discussion also reflects uncertainty regarding the relationship between surface area and pressure differential.

Swamp Thing
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Why doesn't the balloon burst in this video? To me it seems that the differential (guage) pressure between inside and outside the balloon is what matters, and I would think it would be the same as a balloon inflated in the usual way.

https://youtube.com/shorts/3HZ0JkgtpDU?feature=share
 
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Maybe the pressure difference is not large enough for the tensile strength of the balloon material to be exceeded?
 
Isn't it the case that the inflated surface area of the balloon is a measure of the pressure differential? And the area seems to be such that the balloon would normally burst?
 
Swamp Thing said:
Isn't it the case that the inflated surface area of the balloon is a measure of the pressure differential? And the area seems to be such that the balloon would normally burst?
There are competing effects at work. But no, the surface area is not a good gauge of the pressure differential. Paradoxically, increasing surface area is compatible with decreasing pressure differential.

If you've ever blown up a balloon by mouth, you may note that it is hard at first and easy after.

Rubber makes things more interesting. Rubber extends elastically only so far. Then it stops. A typical balloon is inflated approximately to this limit and has high tension as a result. One assumes that the balloon in the bell jar is not inflated that full. It has low tension as a result.
 
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The curvature and tensile strength matter.
For a curved surface the Young-Laplace equation $$\Delta P=-\gamma (\frac 1 R_1 +\frac 1 R_2)$$ gives Pressure differential in terms the principal radii of curvature and the surface tension

Edit: I put in the minus sign
 
I think this calls for a bit lower-level approach:
 
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Bandersnatch said:
I think this calls for a bit lower-level approach:

So the vacuum setup is just a misleading distraction?
 
I'd say so, yes. The problem is with the assumption that all balloons burst when pierced.
 
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hutchphd said:
The curvature and tensile strength matter.
For a curved surface the Young-Laplace equation $$\Delta P=-\gamma (\frac 1 R_1 +\frac 1 R_2)$$ gives Pressure differential in terms the principal radii of curvature and the surface tension

Edit: I put in the minus sign
For a spherical balloon, the tensile stress in the rubber is $$\sigma=\frac{R}{2h}\Delta P$$where h is the present thickness of rubber. For incompressible rubber, h is related to the initial thickness and radius at low pressure by: $$h=\left(\frac{R_0}{R}\right)^2h_0$$
 
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  • #10
I think @Chestermiller's answer to the original question is the correct one. I have done this demonstration using what I called a "funny balloon" which the class quickly recognized as a condom. The darn thing filled the entire available volume without bursting until it was constrained from further expansion by the bell jar wall.
 
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  • #11
Swamp Thing said:
the differential (guage) pressure between inside and outside the balloon is what matters
It is and the maximum exterior 'suck' you can get is when ambient pressure is 0Bar. At that stage, the internal air will have expanded somewhat and what started as 1Bar will have reduced considerably so the pressure difference will be a lot less than -1Bar. Simple Boyle's Law would suggest that an increase in internal volume of 4 would produce a pressure difference of 0.25Bar - and so on. At some stage the envelope will be stressed but not enough to rupture it.
This is very different from the situation where you can use a pump to increase the internal pressure to however much the pump can provide (even your lungs) and that can easily (if you have the nerve) burst the balloon.
It's quite hard to measure the difference between a Good Vacuum and a Deep Vacuum.
kuruman said:
The darn thing filled the entire available volume without bursting until
The embarrassing question is why a condom should ever be required to stretch that far! Not by me, your honour.
 
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