Moderated Continuation - Why a one-way Crush down is not possible

Tony,

Szamboti_Legge said:
As the steel sags two things will happen: the columns, as they shorten, will become wider, which is obvious; and the inherent strength of the steel will increase, which is not obvious. It is well established however that the yield strength of steel increases as the degree of distortion increases. This tendency increases with rising temperature and is pronounced at the temperatures required for collapse, as can be seen in the graph below. 9 For both of these reasons the initial sag cannot be catastrophic but will be very slow and the rate will depend on the rate of heat input. A rising temperature will be needed to offset both the significant increase in yield strength and the slight increase in cross-section area, if collapse is to progress. It is clear therefore that the upper section should only have moved down slowly and only continued to do so if additional heat was supplied. A slow, protracted, and sagging collapse was not observed however with either tower.


picture.php



This is a pretty tortured paragraph. Do you still stand behind it? Or would you care to rephrase it.

Because, I gotta tell ya, that graph doesn't show anything like what you claimed it shows.

Even if it were for A36...

Tom
 
Call me crazy but once something begins to buckle from creep behavior, it doesn't take as much load to buckle it even more. I'm a little curious if this same stance is something he still upholds (the article itself is a bit old).
.
OK. "You're crazy."

But you aren't wrong.

Below is, on the left, is a CORRECT graph of load vs deflection for a buckling column. The force that the column can generate goes rapidly to a very low number & stays there.

picture.php


This chart is from Bazant's reply to Greg Szuladzinski in his "D25, Discussion of "Mechanics of Progressive Collapse: Learning from World Trade Center and Building Demolitions” by Zdenek P. Bažant and Mathieu Verdure
March 2007, Vol. 133, No. 3, pp. 308–319.

The chart on the right is Mr. Szuladzinski's, in which he made two gross errors: 1. claiming that a column had about 4x as much strength as it really did, and 2. once it had buckled in two, suddenly the column magically gained TWICE the load carrying capacity that it had when it was straight. Amazing...

The chart on the right, above, is Mr. Sz's curious guess regarding how he thought the column should behave.

Go figure...


Tom
 
Well, sometimes an element buckles a little and the force causing it slips off (due to the buckle) or decides to buckle something else and the result is just a partly buckled element. Look at any car crash! Plenty of partly buckled elements.

BTW Have you ever seen a one-way car crush down? One car A being crushed by another car C (of similar brand) and A is completely one-way crushed while C just goes off unscated?

Just push on a straw.
 
In 1-D or 3-D? And what is pushing?

I found the pragraph below in a wikipedia article. When each floor of part C inmpacted the upright columns of part A the force was applied and then suddeny released as the column broke through the floor. This hapened for each of the 13 collapsing floors. Does this mean that the on/off nature of the impacting floors on the columns would have contrived to make the upstanding columns effectively stronger ?

''Dynamic buckling
If the load on the column is applied suddenly and then released, the column can sustain a load much higher than its static (slowly applied) buckling load. This can happen in a long, unsupported column (rod) used as a drop hammer. The duration of compression at the impact end is the time required for a stress wave to travel up the rod to the other (free) end and back down as a relief wave. Maximum buckling occurs near the impact end at a wavelength much shorter than the length of the rod, at a stress many times the buckling stress if the rod were a statically-loaded column. The critical condition for buckling amplitude to remain less than about 25 times the effective rod straightness imperfection at the buckle wavelength is
σL = ρc2h
where σ is the impact stress, L is the length of the rod, c is the elastic wave speed, and h is the smaller lateral dimension of a rectangular rod. Because the buckle wavelength depends only on σ and h, this same formula holds for thin cylindrical shells of thickness h.[4]....''

http://en.wikipedia.org/wiki/Buckling
 
Part A, the part of the building above the collapse point, crushes down part B, the single floor below that could never dream of supporting the weight and adds it to its mass. It then crushes down the next part B, the single floor below that and adds IT to its mass. On and on it goes until there all the part B's are gone.

Heiwa. If I can get it, ANYBODY can.
 
You see, tfk, that it is impossible that a structure like WTC 1, 2 one-way crushes down due to local failures due to fire or whatever. I know that you have not understood it so far, but you'll learn.

I hope any NYFD members follow this thread and inform their colleagues! Or invite me to explain that simple fact. My business is of course safety at sea but I also offer my know-how for shore based people.


Vincent Dunn, FDNY buildings collapse expert, would be very surprised to hear you explain that the towers couldn't have collapsed, or whatever it is you say about the towers. It's not really clear.
Report From Ground Zero; Page 310
http://snurl.com/j54ud [books_google_com]

(we can't cut/paste from google books.)

In Report From Ground Zero (pgs 310-311), FDNY structures expert Vincent Dunn describes how the WTC towers had effectively no fireproofing when compared to the older steel buildings, built to standards that required 2 inches of brick and masonry on all structural steel. Dunn also says that the WTC towers were unique in the minimal fireproofing.

Who is Vincent Dunn?
http://unjobs.org/authors/vincent-dunn
 
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Tony,

http://www.internationalskeptics.com/forums/picture.php?albumid=176&pictureid=1436


This is a pretty tortured paragraph. Do you still stand behind it? Or would you care to rephrase it.

Because, I gotta tell ya, that graph doesn't show anything like what you claimed it shows.

Even if it were for A36...

Tom
Don't hold your breath, Tom. It must have been two years ago that I challenged Szamboti to defend his claims in that "peer reviewed" paper in a public debate here against me, a tour guide. He first accepted, then fled like a scared bunny. I'm sure he'll fare much better against Ryan Mackey on Hardfire...in two years he's achieved an understanding of the difference between a column and a beam!
 
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.
OK. "You're crazy."

But you aren't wrong.

Below is, on the left, is a CORRECT graph of load vs deflection for a buckling column. The force that the column can generate goes rapidly to a very low number & stays there.

http://www.internationalskeptics.com/forums/picture.php?albumid=176&pictureid=1437

This chart is from Bazant's reply to Greg Szuladzinski in his "D25, Discussion of "Mechanics of Progressive Collapse: Learning from World Trade Center and Building Demolitions” by Zdenek P. Bažant and Mathieu Verdure
March 2007, Vol. 133, No. 3, pp. 308–319.

The chart on the right is Mr. Szuladzinski's, in which he made two gross errors: 1. claiming that a column had about 4x as much strength as it really did, and 2. once it had buckled in two, suddenly the column magically gained TWICE the load carrying capacity that it had when it was straight. Amazing...

The chart on the right, above, is Mr. Sz's curious guess regarding how he thought the column should behave.

Go figure...


Tom

Nevermind....
 
Part A, the part of the building above the collapse point, crushes down part B, the single floor below that could never dream of supporting the weight and adds it to its mass. It then crushes down the next part B, the single floor below that and adds IT to its mass. On and on it goes until there all the part B's are gone.

Heiwa. If I can get it, ANYBODY can.

Well, first of Bazant & Co use the following parts (actually they call them blocks):
C - upper part/block/assembly of elements above fire zone
A - lower part/block/assembly of elements below fire zone
B - rubble/compacted loose elements of A apparently compacted by C

C is assumed rigid, i.e. it will not change its shape in the process.
A is assumed to break up in the process.
B - how rubble can be regarded as a 'block' of anything is unclear but according Bazant and Co this block (!) can also break up (down!) A.

If you read my papers you'll find that I suggest that C cannot be assumed rigid. This is normal in structural damage analysis.

The result will then be that C is subject to local failures in the process (at the contact interface C/A), which is arrested pretty quickly. No part B will be formed as locally failed/broken elements are still connected to A and C. Thus all masses remain constant and cannot be removed from one part and added to another.

Dynamic buckling of columns will not take place, e.g. a column in A failing due to impact by an element in C! Reason is that the element in C fails, when contacting the column in A; the columns are the strongest elements in the assemblies. You'll not find any buckled columns in the rubble of WTC 1. Actually only the very weak (in shear) end connections of all perimeter columns seem to have failed (they were just bolted together) and in my view the cause for that is controlled demolition. Same for all other failures.
 
Tony,




[qimg]http://www.internationalskeptics.com/forums/picture.php?albumid=176&pictureid=1436[/qimg]


This is a pretty tortured paragraph. Do you still stand behind it? Or would you care to rephrase it.

Because, I gotta tell ya, that graph doesn't show anything like what you claimed it shows.

Even if it were for A36...

Tom

Are you saying that you don't think the graph shows that it takes more energy to further deform the column once it is in the plastic range?
 
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Don't hold your breath, Tom. It must have been two years ago that I challenged Szamboti to defend his claims in that "peer reviewed" paper in a public debate here against me, a tour guide. He first accepted, then fled like a scared bunny. I'm sure he'll fare much better against Ryan Mackey on Hardfire...in two years he's achieved an understanding of the difference between a column and a beam!

Your seemingly continuous need to attempt to slur those you don't agree with makes you look pathetic Mark.

Why don't you at least try to argue the science?
 
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Your seemingly continuous need to attempt to slur those you don't agree with makes you look pathetic Mark.

Why don't you at least try to argue the science?

In my opinion it only takes a critical force to initiate Euler buckling of a slender column. As long as this force does not displace, no energy is applied. As soon as 'buckling' starts, i.e. the column mid-part deflects sideways and the top displaces down, energy is applied (the force displaces down) and energy is absorbed (the column displaces sideways and actually heats up a little).
As no column can really be regarded as 'slender' or just a 1-D line, we have to accept that the column is 3-D and thus does not just deflect sideways, while the top displaces down. It also compresses and deforms unsymetrically and plastic hinges will develop in the column. All those effects require energy and one question is whether the critical force that initiated the 'buckling' is suffient to continue the 'buckling' - assuming that the force does not just slip off.
There are many examples of columns that have started to 'buckle' - actually deformed in 3-D - due to a force applied and then reached a new 'damaged state' equilibrium still carrying the initial force applied. It simply means that the damaged/buckled column is stronger than the intact column. I would expect that should have occurred on 911.

Now, let's assume the force/energy is available to really rip the 'buckled' column apart in two pieces, i.e. a plastic hinge develops 100% through the column and then the material fractures straight through. Evidently only ONE such fracture can develop in any column and then the upper and lower fractured surfaces of the broken column have to find something else to rest on so that the force applied can try to destroy those elements. They will probably be elements adjacent to the broken column, e.g. floors!

As explained many times, I assume that the two broken ends of the column will thus punch holes in the floors they meet. It means, i.a. that the upper floors are subject to damage. Anyone suggesting that the upper floors can buckle columns below has not really understood the process.
 
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[/QUOTE] Is this the footprint ofWTC1 ?

FEMA photographer Kurt Sonnenfeld (recently interviewed by Voltairenet) has released a new set of World Trade Center disaster site images. Some were previously available, but the majority are new and high quality.

http://www.911blogger.com/node/20461
 
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Tony,

Are you saying that you don't think the graph shows that it takes more energy to further deform the column once it is in the plastic range?

No, I'm not saying anything like that. And neither did you in the paragraph that I quoted.

Here's what you said.

Szamboti_Legge said:
As the steel sags two things will happen: the columns, as they shorten, will become wider, which is obvious; and the inherent strength of the steel will increase, which is not obvious. It is well established however that the yield strength of steel increases as the degree of distortion increases. This tendency increases with rising temperature and is pronounced at the temperatures required for collapse, as can be seen in the graph below. 9 For both of these reasons the initial sag cannot be catastrophic but will be very slow and the rate will depend on the rate of heat input. A rising temperature will be needed to offset both the significant increase in yield strength and the slight increase in cross-section area, if collapse is to progress. It is clear therefore that the upper section should only have moved down slowly and only continued to do so if additional heat was supplied. A slow, protracted, and sagging collapse was not observed however with either tower.


Here's the graph:
picture.php


These are the most important things that the graph shows:
1. The yield strength (stress level at which the curve first deviates from linear) decreases with increasing temp
2. The ultimate strength (max stress level) decreases with increasing temp.
3. The elastic modulus (slope of the initial linear portion of the curve) decreases with increasing temp.

My gut feel tells me that the third item played the largest role in the collapse of the towers.

Now, I'll leave it to you to explain why you guys published curves for A43 instead of for A36. It's not like the right curves were not available.

A36 Stress Strain Curve
picture.php


With regard to the comments:
Szamboti_Legge said:
As the steel sags two things will happen: the columns, as they shorten, will become wider, which is obvious and the inherent strength of the steel will increase, which is not obvious.

This is only true if the columns stay almost perfectly straight. As soon as they begin to bow, which in the towers happens very quickly, this effect becomes irrelevant.

Szamboti_Legge said:
It is well established however that the yield strength of steel increases as the degree of distortion increases.

And this is your key claim. It is wrong.

The yield strength, the stress level at which the curve deviates from linear (or for steels with gradual elastic-plastic transition regions, the stress level that produces 0.2% residual strain when unloaded) is unrelated to "distortion levels". Strain is the independent variable. And the yield strength is DEFINED as occurring at one single, specific point on the stress strain curve. (The FIRST such point on a non-monotonic curve.) Ergo, by definition, it does not, and can not change its location on this curve as a function of the independent variable.

Szamboti_Legge said:
This tendency increases with rising temperature and is pronounced at the temperatures required for collapse, as can be seen in the graph below.

Well, the tendency doesn't occur. So it's not at all visible in that graph. If you think that it is, I'd be happy for you to point it out to me & explain your interpretation.

Szamboti_Legge said:
For both of these reasons the initial sag cannot be catastrophic but will be very slow and the rate will depend on the rate of heat input.

"the initial sag cannot be catastrophic...?" Parts made of structural steel cannot fracture? I disagree.

Szamboti_Legge said:
A rising temperature will be needed to offset both the significant increase in yield strength and the slight increase in cross-section area, if collapse is to progress.

Except that there is no "significant increase in yield strength". And when the progressive tilting of the building was occurring, it was happening due to bending of the vast majority of the columns, not pure compression of virtually any of the columns.

And this statement is absolutely, 100% wrong. It is wrong because you have been considering only the short term stress-strain curve. If you were to add a time axis to your stress-strain curve, you'd find that runaway, progressive, catastrophic creep can happen at very low temperatures. As Bazant, et al, showed, you can get progressive, catastrophic creep at temperatures as low as 150°C.

You most certainly do NOT have to put in "rising temperature" to get unlimited creep and failure. The reality is exactly the opposite.

Bazant showed that creep rate is crucially dependent on the stress level. At high stress levels, runaway creep can occur at remarkably, unexpectedly low temperatures.

The consequence of this fact is that, since the stress levels increase as the building's tilt increases, then a constant temperature (at increasing stress levels) will produce a progressively FASTER creep. The building's progressive tile causes it to race towards catastrophe faster & faster, even at a constant temperature.

Szamboti_Legge said:
It is clear therefore that the upper section should only have moved down slowly and only continued to do so if additional heat was supplied. A slow, protracted, and sagging collapse was not observed however with either tower.

Wrong. The tower did not "sag down slowly". It tilted to the side. As it did, it put bending stresses into components that were never designed to withstand them. Pieces fractured continuously, but other parts were able to take up the load for the lost piece. Finally, there was no margin left. Some last part failed, the other components were unable to take up the load of that last, lost part, they failed, more failed and the cascade led to runaway failure.

The last, catastrophic failure was NOT "temperature mediated". It was a physical failure, specifically sudden buckling. Temperature brought the building to this failure point, but the failure itself was a sudden mechanical fracture. And nobody expects "slow, protracted, sagging collapse" out of fractures.

There is no mystery here, Tony.
 
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