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Originally posted by HowardRoark
Eutectic mixtures (i.e. hot corrosion) occur at relatively low temperatures. Generally less than 1000 C.
www.me.wpi.edu...
All of those steel pieces were pulled out of the rubble weeks after the collapse.
Originally posted by Skadi_the_Evil_Elf
But you still havent explained what evaporated the steel.
Limited Metallurgical Examination (pdf)
Evidence of a severe high temperature attack on the steel, including oxidation and sulfidation with subsequent intergranular melting, was readily visible in the near-surface microstructure. A liquid eutectic mixture containing primarily iron, oxygen, and sulfur formed during this hot corrosion attack on the steel. This sulfur-rich liquid penetrated preferentially down grain boundaries of the steel, severely weakening the beam and making it susceptible to erosion. The eutectic temperature for this mixture strongly suggests that the temperatures in this region of the steel beam approached 1,000 °C (1,800 °F), which is substantially lower than would be expected for melting this steel.
Originally posted by Clark_Kent
That's something else. If you have something that shows 3000C then show me.
The specific steel Barnett was talking about didn't reach 1000C.
Maybe you can tell me why Jones bring up 5,000 degree temps when we know the steel Barnett was talking about didn't get close.
Originally posted by Skadi_the_Evil_Elf
Since I cannot see any reason why Barnett would make such a thing up, and since the wreckage was hauled off too quickly for others to analyize, I see no reason to dispute Barnett's assertion that the steel had partially vaporized.
Originally posted by Skadi_the_Evil_Elf
www.physics.byu.edu...
And of Course, professor Jones seems to believe that Barnett was correct as well.
Originally posted by St Udio
if one goes back to the FEMA pdf link which started the thread,
and one looks at page 8 of 13 (increase the size of print)
you can read two sulfidated samples are deemed steel from towers 1 & 2
and the (heat?)-evaporated A36 steel was from WTC7
Limited Metallurgical Examination (pdf)
Page C-8:
Figure C-13 shows the region where a qualitative chemical analysis of the eroded region was performed. The comparison of the EDX spectra from the specific regions identified in Figure C-13 shows concentration of copper and sulfur in the grain boundaries in addition to iron sulfide formation adjacent to iron oxide in the oxidized surface layer. Sulfide formation within the steel microstructure increases in concentration as the oxidized region is approached from the steel side. This is clearly shown in Figure C-14.
The larger sulfides further into the steel are the more stable manganese sulfides that were formed when the steel was made. The smaller sulfides that have formed as a result of the fire do not contain significant amounts of manganese, but rather are primarily sulfides containing iron and copper. These sulfides have a lower melting temperature range than manganese sulfide. It is much more difficult to tell if melting has occurred in the grain boundary regions in this steel as was observed in the A36 steel from WTC 7. It is possible and likely, however, that even if grain boundary melting did not occur, substantial penetration by a solid state diffusion mechanism would have occurred as evidenced by the high concentration of sulfides in the grain interiors near the oxide layer. Temperatures in this region of the steel were likely to be in the range of 700-800 °C (1,290-1,470 °F).
(Image resized for posting.)
Originally posted by St Udio
but the way the information is packaged & presented,
one is led to infer that the type of damaged steel in WTC7
is assumed to be found in the steel from towers 1 & 2.
...and vise-versa...
which is so NOT the case
2 different types of structures & construction
2 different causes for the collapses
Originally posted by HowardRoark
There was adequate fuel and oxygen for the fires to burn.
1000 C is well within the ordinary temperature range of a fire.
Originally posted by HowardRoark
For every floor, consider the carpet, and or floor tile, add in the fabric, foam, plastic and wood of the cubicles. Add in the plastic of the computers and the miles of cables, add in the file cabinets, drawers full of paper.
Originally posted by HowardRoark
Fuel starved?
For every floor, consider the carpet, and or floor tile, add in the fabric, foam, plastic and wood of the cubicles. Add in the plastic of the computers and the miles of cables, add in the file cabinets, drawers full of paper.
Seems like a lot of fuel to me.
Originally posted by bsbray11
It's also extremely unlikely that the hydrocarbon fuel at the site could have caused steel to melt post-collapse in any scenario that isn't really pushing credibility.
Originally posted by bsbray11
1000 C is well within the ordinary temperature range of a fire.
This is a lie and you know it.
Hydrocarbon fires won't burn much more than 800 degrees Celsius absolute max, except for flashovers, which are very brief and not sustained, and certainly not for weeks. That is insane.
Even 800 degree or so hydrocarbon fires are only possible when the best conditions are available.
Pants On Fire
before V0.84: the page The Fires stated: 800º C is near the maximum temperature at which hydrocarbons will burn in air at sea level: 825º C." This implies that 825º C is a theoretical upper limit on flame temperatures in hydrocarbon fires, when in fact such fires may reach much higher temperatures when fed pressurized or pre-heated air. Of course in a building fire, there is unlikely to be any pressurized air, and pre-heating of air is limited by the fact that the fires continuously draw in fresh air. An exception is flash-over, in which pre-heated gases suddenly ignite, sometimes reaching temperatures over 900º C. This is a momentary phenomenon, however, and will not produce sustained fire temperatures this high.
The maximum temperature would have been 1,600°F or 1,700°F. It's impossible to generate temperatures much above that in most cases with just normal fuel, in pure air. In fact, I think the World Trade Center fire was probably only 1,200°F or 1,300°F.
Investigations of fires in other buildings with steel have shown that fires don't usually even melt the aluminum, which melts around 1,200°F. Most fires don't get above 900°F to 1,100°F. The World Trade Center fire did melt some of the aluminum in the aircraft and hence it probably got to 1,300°F or 1,400°F.
Are you disputing Dr. Barnett's findings, suggesting that some fuel other than what would normally have been expected in the WTC melted the steel, or some other possibility I'm unaware of?
Originally posted by bsbray11
Pants On Fire
Who exactly are you suggesting is lying here? Btw, what is up with these things anyway?
Originally posted by bsbray11
Pants On Fire
Who exactly are you suggesting is lying here? Btw, what is up with these things anyway?
Originally posted by bsbray11
This is a lie and you know it.
Originally posted by billybob
it's magically debasing!
say, majic, you seem to be off the mccarthyistic witch hunt, and onto a selective science bent, complete with ridicule of opposing views.
QUESTION FOUR:
would you be willing to except alternative interpretations or views without calling your opponents liars?
A thermodynamic analysis of the Fe-S-O system is currently underway to determine the atmosphere that would form these sulfidation/oxidation products. In addition, these microstructural observations will be compared with results from steels in various furnace and petrochemical processes.
Originally posted by bsbray11
Originally posted by HowardRoark
1000 C is well within the ordinary temperature range of a fire.
This is a lie and you know it.
Hydrocarbon fires won't burn much more than 800 degrees Celsius absolute max, except for flashovers, which are very brief and not sustained, and certainly not for weeks. That is insane.
Even 800 degree or so hydrocarbon fires are only possible when the best conditions are available.
When one consults combustion textbooks for the topic of 'flame temperature,' what one normally finds are tabulations of the adiabatic flame temperature. 'Adiabatic' means without losing heat. Thus, these temperatures would be achieved in a (fictional) combustion system where there were no losses. Even though real-world combustion systems are not adiabatic, the reason why such tabulations are convenient is because these temperatures can be computed from fundamental thermochemical considerations: a fire experiment is not necessary. For methane burning in air, the adiabatic flame temperature is 1949°C, while for propane it is 1977°C, for example. The value for wood is nearly identical to that for propane. The adiabatic flame temperatures for most common organic substances burned in air are, in fact, nearly indistinguishable. These temperatures are vastly higher than what any thermocouple inserted into a building fire will register!
There is fairly broad agreement in the fire science community that flashover is reached when the average upper gas temperature in the room exceeds about 600°C. Prior to that point, no generalizations should be made: There will be zones of 900°C flame temperatures, but wide spatial variations will be seen. Of interest, however, is the peak fire temperature normally associated with room fires. The peak value is governed by ventilation and fuel supply characteristics [12] and so such values will form a wide frequency distribution. Of interest is the maximum value which is fairly regularly found. This value turns out to be around 1200°C, although a typical post-flashover room fire will more commonly be 900~1000°C. The time-temperature curve for the standard fire endurance test, ASTM E 119 [13] goes up to 1260°C, but this is reached only in 8 hr. In actual fact, no jurisdiction demands fire endurance periods for over 4 hr, at which point the curve only reaches 1093°C.
The peak expected temperatures in room fires, then, are slightly greater than those found in free-burning fire plumes. This is to be expected. The amount that the fire plume's temperature drops below the adiabatic flame temperature is determined by the heat losses from the flame. When a flame is far away from any walls and does not heat up the enclosure, it radiates to surroundings which are essentially at 20°C. If the flame is big enough (or the room small enough) for the room walls to heat up substantially, then the flame exchanges radiation with a body that is several hundred °C; the consequence is smaller heat losses, and, therefore, a higher flame temperature.