You are saying that a level can be crushed by 38% of its static load capacity because that is the force you are applying which is the AVERAGE over the collapse of that level.
Correct. This is the so-called "Maxwell construction", a physical law of nature, expressed in a simple mathematical form, and borne out each and every time by experiment. It only applies when the supports are completely crushed. If the stories are crushed (and a couple of other conditions are true, which I will explain only if you're interested) it is a valid means of doing the dynamics of crushing a level.
It had to have been designed to hold more than that AVERAGE but you are multiplying that force times the height of the level to get the amount of energy expended to do the collapse ACCORDING TO YOUR ASSUMPTION.
It's not an assumption, it's a fucking law of nature - one which you are ignorant of.
This brings us to... what happens if there isn't sufficient energy to crush a level? Then the Maxwell construction can't be used.
You are choosing not to question if the PEAK FORCE can be reached at every level.
Number one astute observation you've made recently, perhaps in forever.
Correct, I am choosing not to question if the peak force can be reached at every level. But you wouldn't know that from the graphs, because they don't tell that story. All of my computational environments are capable of accounting for peak force, only one of them allows me to choose not to! All of them give results which agree to story level detail, whether the Maxwell construction is used in the one environment or not.
There are three environments:
1) A storywise crush calculator (discrete algebraic model)
2) A physics engine
3) A extended finite element program
The first only supports a rigid top, because two degree of freedom calculations (that is, where the upper block can crush too) cannot be done in the discrete algebraic method. The other two can support non-rigid tops but do not have the overall flexibility of the first. They can also suffer from being too realistic sometimes (example: the vibration you had a cow over is actually quite realistic for 1kg metallic masses in collision - you ever heard metal ringing? Duh). I end up with an artifact of the test configuration rather than a demonstration of a fundamental principle.
Therefore I frequently use the first environment, even though it can't do a collapsing upper block and despite its story resolution limit. I programmed this (many times, many ways) myself, and I've included a setting to indicate whether to run with a Maxwell line equivalent average force over an entire story, or to section the story into elastic, peak plastic, and minimum plastic step value approximations to the actual chosen load displacement. This is not as precise as the other two environments, which are both iterative force/constraint solvers of different architectures, but it is sufficient to establish arrest or no arrest at each level.
That's not to say the Maxwell line option can't arrest. When I model your model, I use the Maxwell line and I come up with the same number of stories crushed, only mine are necessarily all in the bottom block when using the first method. It arrests just fine.
If I know that there's no way a particular configuration will approach arrest, based on more detailed runs, I use the Maxwell line. After all these trials, I have a pretty good feel for what will arrest. From a theoretical standpoint, it's very simple: Maxwell line above mg arrests, everything else doesn't. Constant FOS or DCR means the same Maxwell line AND DCR at every level, so that's a no-brainer. If it gets over the peak in the first collision,
by definition it will get over every subsequent peak.Your model has an average Maxwell line above mg; that's WHY it arrests. There's no other reason, it's not a fucking mystery. I knew that before making the loops and load testing them. The loops crush by deforming into a
slightly stronger structure when at minimal compaction. You basically wiped out the peak, barely strong enough to stand, but with...
A MAXWELL LINE ABOVE MG!
The questions were:
- is it strictly the resistance of the loops as resistive force, or were vibration/friction/air expulsion sinks necessary to achieve arrest?
- what was the approximate load-displacement curve for paper loops?
The measurements answered these questions. Make it strong enough (or in your case, spongy enough), it will arrest.
PS - the Maxwell line technically CANNOT be used to model your model for the reasons I haven't yet discussed; nevertheless, it's so good that it comes close enough, anyway.