Q: Would you rather land on water or marshmallow?

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Discussion Overview

The discussion centers around the hypothetical scenario of landing on water versus a cushion of marshmallow in the absence of a parachute, particularly in the context of skydiving and bungee jumping. Participants explore the physical properties of both landing surfaces, including factors like surface tension, density, and compressibility, while considering the implications of high-altitude falls.

Discussion Character

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

Main Points Raised

  • Some participants argue that landing on marshmallow would be preferable due to its compressibility compared to the incompressibility of water, which can be lethal from great heights.
  • Others highlight the importance of density and compressibility in determining the safety of landing on marshmallow versus water.
  • A participant with skydiving experience mentions that terminal velocity is reached at about 120 MPH, regardless of jump height.
  • There are discussions about the potential for marshmallow to behave like quicksand, complicating escape after landing.
  • Several participants propose calculations regarding the depth of marshmallow required to safely cushion a fall from significant heights, considering factors like terminal velocity and spring constants.
  • One participant humorously suggests that a theme park based on marshmallow could be a viable idea, while others engage in light-hearted banter about the implications of such a concept.

Areas of Agreement / Disagreement

Participants express a variety of opinions on the safety and feasibility of landing on marshmallow versus water, with no consensus reached on which option is definitively better. The discussion remains unresolved with multiple competing views and hypotheses presented.

Contextual Notes

Participants mention various assumptions, such as the conditions at impact and the properties of marshmallow, but these remain unresolved. The calculations proposed depend on specific values for spring constants and other variables that are not universally agreed upon.

Who May Find This Useful

This discussion may be of interest to those curious about physics, particularly in the context of impact forces, material properties, and hypothetical scenarios in extreme sports.

  • #31


tiny-tim said:
But is marshmallow springy …

does it return to its original shape?

If not, then "spring constant" isn't the issue.

A spring absorbs energy, and then returns it …

a "crumple zone" absorbs energy, but keeps it …

I thought that was why MattSimmons :smile: chose marshmallow in the first place?
That is why I assumed a constant rupture force rather than a spring model.
 
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  • #32
i can stop by the local Tractor Supply store and pick up some 1/2 inch washers..these are about the size of a half dollar. if i stack these , one a t a time, we should see when the marshmellow collapses ..this the stree ruoture rate you were talking about?
any other advise on method to use?
freeze um first?
do i need my infrared pyrometer too?
 
  • #33


tiny-tim said:
But is marshmallow springy …

does it return to its original shape?

If not, then "spring constant" isn't the issue.

A spring absorbs energy, and then returns it …

a "crumple zone" absorbs energy, but keeps it …

I thought that was why MattSimmons :smile: chose marshmallow in the first place?

So it would be a landing zone that doubles as a trampoline! Sounds fun! :P
 
  • #34
rupture force

Hi DaleSpam! :smile:
DaleSpam said:
That is why I assumed a constant rupture force rather than a spring model.

ah, i missed that … you posted it just before my last post

but what is rupture force (it doesn't sound very nice :frown:)?

i wiki'ed it, but couldn't find anything. :redface:
DyslexicHobo said:
So it would be a landing zone that doubles as a trampoline! Sounds fun! :P

hmm … that's what was bothering me :redface:

falling 20,000 feet onto a trampoline doesn't seem much better than crashing! :biggrin:

:rolleyes: boinggg! boinggg! :rolleyes:
 
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  • #35


tiny-tim said:
but what is rupture force (it doesn't sound very nice :frown:)?
It is point number 3 on this http://en.wikipedia.org/wiki/Stress-strain_curve" (Figure 1). Basically, it is the point where the material breaks, complete failure.

So, to measure it you would push on a marshmallow until it failed and measure the force and the area that you were pushing.
 
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  • #36
rupture force and viscosity

DaleSpam said:
It is point number 3 on this http://en.wikipedia.org/wiki/Stress-strain_curve" (Figure 1). Basically, it is the point where the material breaks, complete failure.

So, to measure it you would push on a marshmallow until it failed and measure the force and the area that you were pushing.

ah … got it! :biggrin:

so below the rupture force, the marshmallow will act to some extent like a spring, returning MattSimmons upward with a fairly high overall deceleration,

but beyond the rupture force, the marshmallow will continuously give way, providing a relatively safe steady viscous deceleration? :smile:

hmm … so now we also need to know the viscosity of marshmallow? :confused:

and presumably it would help to be covered with chocolate, or with some other material that will reduce marshmallow drag? :wink:
 
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  • #37
those marshmallows are tuffer than I thought. got a bag of Wal-Mart Great Value Marshmallows..these are the biggies..weigh 6 grams, 3 mm tall 30.2 mm diameter
did the measurements when they were 64 degrees..were in trunk over night
I stacked various washers on top until one side of the marshmallow wall gave in..I was not yet able to load the marshmallow to blow it out.total collapse.
in fact , I was only able to load 540 gram max load and the darn thing still did not fail to return to 3 mm height after load. I have to find some bar stock of sufficient weight to mash it
the height is from edge of a dished washer to the desk top and measured with a pocket scale ..note i used the slider bar on the pocket scale


the following was with washers perfectly balance

load - height mm
0 - 3.0
50 - 2.8
85 - 2.4
102 - 2.2
150 - 2.1
215 - tilt, side wall failure


I has to steady the washers by holding them so side wall would not collapse

load - height in mm
0 - 2.2
140 - 2.0
210 - 1.8
280 - 1.7
540 - 1.3
824 - 1.2
 
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  • #38
Ranger Mike said:
those marshmallows are tuffer than I thought. got a bag of Wal-Mart Great Value Marshmallows..these are the biggies..weigh 6 grams, 3 mm tall 30.2 mm diameter
did the measurements when they were 64 degrees..were in trunk over night
I stacked various washers on top until one side of the marshmallow wall gave in..I was not yet able to load the marshmallow to blow it out.total collapse.
in fact , I was only able to load 540 gram max load and the darn thing still did not fail to return to 3 mm height after load. I have to find some bar stock of sufficient weight to mash it
the height is from edge of a dished washer to the desk top and measured with a pocket scale ..note i used the slider bar on the pocket scale


the following was with washers perfectly balance

load - height mm
0 - 3.0
50 - 2.8
85 - 2.4
102 - 2.2
150 - 2.1
215 - tilt, side wall failure


I has to steady the washers by holding them so side wall would not collapse

load - height in mm
0 - 2.2
140 - 2.0
210 - 1.8
280 - 1.7
540 - 1.3
824 - 1.2
How big are the marshmallows? 1" in diameter by 1" tall? If so, using 215 g/in² (most marshmallows will probably fail this way rather than rupture), and a surface area of .7 m² (good for 74 kg adult male, so a little conservative for a 100 kg man) we get a revised force of 2300 N which is a little more than double my previous guesstimate. So 180 kJ/2300 N = ~ 80 m. Multiply by a factor of 2.5 for safety and call it 200 m of marshmallows.
 
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