Jonnyclueless
Philosopher
- Joined
- Jun 18, 2007
- Messages
- 5,546
Thanks that makes sense. But why doesn't the truth movement mention that information? Why do they leave such details out?
The interesting thing is that the 35-foot truss that failed the 2-hour rating was restrained – pinned at each end – as it would be in a real building. Its failure was a surprise to researchers and led to much further research.Hi Jonnyclueless,
Tests were performed to see if the floor assemblies were compliant with the ASTM E 119 standard for fire resistance. These tests were performed on fire-insulated trusses. They did sag. Some failed to get a two-hour rating.
http://wtc.nist.gov/NISTNCSTAR1-6B.pdf
Because the only things holding their fantasies together are lies, omissions, and misrepresentations.Thanks that makes sense. But why doesn't the truth movement mention that information? Why do they leave such details out?
I've got pretty much the same figures, unsurprisingly. I don't know how Bazant and Zhou arrived at their estimates. The more recent paper by Bazant, Le, Greening and Benson assumes that the mass is "almost 500,000 tons". They use a distribution (from the top down to the bottom of the bath-tub):
mu(z) = k_0*exp(k_2*z) + k_1
The values of the constants are unspecified. Maybe Apollo20 will inform us.
http://www.democraticunderground.co...mesg&forum=125&topic_id=159282&mesg_id=159611
Carefulplease; said:They did perform tests on full-scale short-span (35 feet) trusses. The largest furnaces available to perform fire tests were those of Underwriters Laboratories of Canada in Toronto. They were able to verify the effects of scale through comparing the results for both full-scale and half-scale tests. To build a 60 feet furnace would have been expansive and would have provided diminishing returns.
For the record, this was inaccurate. This mu function was used from the top to the 81th floor and the rest of the variation was linear all the way down.
Can someone cleverer than I tell me how to solve for k in the expression
c = k*exp(k*z)
where both c and z are numerical constants?
and take the ln (lawn) and solve i believe. ln (c) = k^2z i think, been a whileFor the record, this was inaccurate. This mu function was used from the top to the 81th floor and the rest of the variation was linear all the way down.
Can someone cleverer than I tell me how to solve for k in the expression
c = k*exp(k*z)
where both c and z are numerical constants?
I believe that reduces down by taking the log of both sides. I haven't used logarithms in a long time though.
I just get c = ln(k) + kz.
(k is the only unknown 3bodyproblem)
I looked at my expansion and my head started to hurt with all those terms, so I simplified even more to a two-term expansion which gives us a quadratic equation.
c = k + z*k^2
or
z*k^2 + k - c = 0
Using the quadratic formula, I can now solve for k:
k = (-1 +/- sqrt(1 - 4*z*(-c)))/(2*z)
or
k = {(-1 + sqrt(1 + 4zc))/2z), (-1 - sqrt(1+4zc))/2z)}
I have no idea what this means by now. I hope you can make something of it, Carefulplease!
Thanks for the hard work AZCat. I fear the two-term expansion might deviate too much in the range I am interested with. I might try Newtons Bit poor-man's numerical method and tell you how much yours deviates![]()
Can someone cleverer than I tell me how to solve for k in the expression
c = k*exp(k*z)
where both c and z are numerical constants?
R.Mackey; said:This is a classic transcendental equation.

The correct mass and proper sequence of "crush up" first makes a huge difference in the timings. If Bazant is wrong about the amount of ejected debris this also makes a significant difference. I still think 20% is very low. I think we will find that the gravity driven collapse time will end up being around 20 seconds.
The correct mass and proper sequence of "crush up" first makes a huge difference in the timings.
shagster; said:Based on the height of the rubble pile within the tower footprint and assuming that the stories were squashed down to about 10 to 15% of their original height, a total mass shedding of 20% of the tower mass isn't very low. 20% to 30% shedding is reasonable. When the shedding is higher than 30%, it becomes difficult to explain how the top of the pile could be near the bowtie level, unless the debris in the pit is considered to be loosely compacted.
The collapse duration is relatively insensitive to mass shedding. I've written a Greening type of model that accounts for a constant amount of mass shedding per story impact during crush-down. A total shedding of 30% of the tower mass adds about one second to the collapse duration compared with no shedding. That doesn't put the predicted collapse duration beyond the observed duration.