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Study of Technology for Detecting Pre-Ignition Conditions of ... - NIST

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CPSC-IAG95-1145<br />

Figure 30 shows the total hyh-oca.rlxm ad water areas as a function <strong>of</strong> time fen-a test <strong>of</strong><br />

~~]~ea~e~ on ~ elec~ic range with the range hood <strong>of</strong>f. Hydrocarbon area is the area under the<br />

hydrocarbon spectral peak integrated from 2782 cm-l to 3029 cm-l. Thk frequency range<br />

corresponds to the spectral band produced by the stretching <strong>of</strong> carbon-hydrogen bonds in alkanes,<br />

alkenes, and aromatic hydrocarbons. 9 The limited spectral resolution <strong>of</strong> the instrument and the<br />

likely overlap and interference <strong>of</strong> the spectra <strong>of</strong> many hydrocarbons prevented fi.uther<br />

identification <strong>of</strong> specific organic compounds within the broad peak. The hydrocarbon curve rises<br />

sharply in a manner similar to the laser attenuation curves. The water area is the area under the<br />

water spectral peak integrated from 1644 cm-l to 1755 cm-l. Water increases more gradually<br />

than the hydrocarbons and peaks at one fourth <strong>of</strong> the hydrocarbon amount.<br />

Figure 31 shows a wmparison <strong>of</strong> the hydrocarbon-area measurements <strong>for</strong> all <strong>of</strong> the food<br />

and range-hood combinations heated cm the electric range- Sugar produces similar levels <strong>of</strong><br />

hydrocarbons to those produced by the other foods, but in a shorter period <strong>of</strong> time. The CWVeS<br />

closely resemble those <strong>for</strong> laser attenuation except sugar generates the most hydrocarbons,<br />

followed by bacon and oil.<br />

Figure 32 shows a comparison <strong>of</strong> the hydrocarbon-area measurements <strong>for</strong> all <strong>of</strong> the food<br />

and range combinations heated on the high-output gas range. The gas range seems to produce<br />

similar levels <strong>of</strong> hydrocarbons from heating food to those produced by the electric range. The<br />

coarse time resolution <strong>of</strong> these measurements makes it difficult to accurately compare the<br />

maximum levels since the last spectral scans be<strong>for</strong>e ignition are averaged with scans tier<br />

ignition, The data points shown are those averages that were not tainted by post-ignition scans,<br />

Figure 33 shows a comparison <strong>of</strong> the water-area measurements <strong>for</strong> all <strong>of</strong> the food and<br />

range-hood combinations heated on the electric range. The heating <strong>of</strong> sugar produces much more<br />

water than either bacon or oil due to the breakdown <strong>of</strong> the chemical structure <strong>of</strong> sucrose. For<br />

bacon, water initially boils <strong>of</strong>f due to the water content <strong>of</strong> the meat, and then more water vapor<br />

<strong>for</strong>ms later as a pyrolysis product. Heating <strong>of</strong> the oil produces no water initially, but increasing<br />

amounts <strong>for</strong>m as some components <strong>of</strong> the oil begin to break down.<br />

Figure 34 shows a comparison <strong>of</strong> the water-area measurements <strong>for</strong> all <strong>of</strong> the food and<br />

range combinations heated on the high-output gas range. Water was measured immediately upon<br />

the start <strong>of</strong> each test using the gas range. This is due to the addition <strong>of</strong> a constant level <strong>of</strong> water<br />

vapor from combustion <strong>of</strong> the burner flame to the water contributed from the foods.<br />

~ ef<strong>for</strong>t was made to generate Coz mea cu~es by integrating the C02 SPeCtral band<br />

from 2320 cm-l to 2383 cm-]. The results initially seemed nonphysical because <strong>of</strong> negative areas<br />

which implied a decrease in C02 from ambient levels. One possible explanation is that little or<br />

no air, which contains C02 on the order <strong>of</strong> several hundred ppm, WaS en~ained by the PIume ~d<br />

passed by the FTIR beam in the section <strong>of</strong> the path length over the pan. Thk would cause less<br />

C02 to be measured during the experiments than was measured as background levels. Since the<br />

background data were subtracted from the experimental da@ negative areas resulted. Another<br />

explanation is that the increased temperature <strong>of</strong> the plume relative to the cool background caused<br />

the C02 molecules to spread apart, and the decreased number density <strong>of</strong> COZ molecules was<br />

interpreted as an absolute decrease in C02 by the FTIR. A third possibility is that the increase<br />

in plume temperature during the test over the ambient background temperature produced enough<br />

additional infrared radiation from the plume to cause the relative absorbance by C02 in the hot<br />

49

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