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These locally correlated polar regions would be expected below the Burns temperature of a relaxor or conventional ferroelectric, consistent with the measurement being performed only about 100 K above the structural transition.
In the non-dispersion region below Td (Burns temperature), mean-field theory is applicable.
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This system has the advantage of producing few gaseous products and the burn temperature is far higher than the ignition temperature of the energetic materials used.
By using wavelet packet transforms, AE features at the grinding burn temperature can successfully be extracted without other mechanical interferential factors.
The analysis of the INTOR-plasma shows that at a burn temperature Tb = 10 keV the fusion power (122 MW) exceeds the line radiation, ionization, conduction, and convection losses by 11 MW.
Prior studies stated that the mild burn temperature was 60°C.
This achieved the effect of hyperthermic temperature (37.5 38.3°C), 16 18 while remaining lower than the mild burn temperature (60°C).
Silica polymorph transitions indicate the high burn temperatures of ≈1550 °C, produces ash dominated α −quartz rather than expected α-cristobilite and amorphous silica; although α-cristobilite, and amorphous silica are present.
The obtained dependence of burn rate on burn surface temperature fits the unified gasification law for nitramines.
You're working with a volatile substance that is constantly changing as the fuel burns, outside temperature changes, the speed at which you walk or even the wind changing direction - it's akin to light painting with a dodgy bulb or loose connecting in your light source - however, this is where the fun lies, doing something that's a challenge!
The workers then move them up towards the pit's high ceiling and drop the waste into furnaces built with technology from Germany, Japan and elsewhere.The waste burns at temperatures of 850°C or higher, hot enough to eliminate toxic dioxin pollutants.
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