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Optical Properties of Biomass Burning Aerosols: Comparison of Experimental Measurements and T-Matrix Calculations

机译:生物质燃烧气溶胶的光学性质:实验测量和T矩阵计算的比较

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The refractive index (RI) is an important parameter in describing the radiative impacts of aerosols. It is important to constrain the RI of aerosol components, since there is still significant uncertainty regarding the RI of biomass burning aerosols. Experimentally measured extinction cross-sections, scattering cross-sections, and single scattering albedos for white pine biomass burning (BB) aerosols under two different burning and sampling conditions were modeled using T-matrix theory. The refractive indices were extracted from these calculations. Experimental measurements were conducted using a cavity ring-down spectrometer to measure the extinction, and a nephelometer to measure the scattering of size-selected aerosols. BB aerosols were obtained by burning white pine using (1) an open fire in a burn drum, where the aerosols were collected in distilled water using an impinger, and then re-aerosolized after several days, and (2) a tube furnace to directly introduce the BB aerosols into an indoor smog chamber, where BB aerosols were then sampled directly. In both cases, filter samples were also collected, and electron microscopy images were used to obtain the morphology and size information used in the T-matrix calculations. The effective radius of the particles collected on filter media from the open fire was approximately 245 nm, whereas it was approximately 76 nm for particles from the tube furnace burns. For samples collected in distilled water, the real part of the RI increased with increasing particle size, and the imaginary part decreased. The imaginary part of the RI was also significantly larger than the reported values for fresh BB aerosol samples. For the particles generated in the tube furnace, the real part of the RI decreased with particle size, and the imaginary part was much smaller and nearly constant. The RI is sensitive to particle size and sampling method, but there was no wavelength dependence over the range considered (500?¢????680 nm). Our values for the RI of fresh (white pine) biomass burning aerosols ranged from 1.33 + i0.008 to 1.74 + i0.008 for 200-nm, 300-nm, and 400-nm diameter particles. These are within the range of RI values in the most recent study conducted during the Fire Laboratory at Missoula Experiments (FLAME I and II), which were 1.55 to 1.80 for the real part, and 0.01?¢????0.50 for the imaginary part, for fresh BB aerosols with diameters of 200?¢????570 nm. There is no clear trend on the dependence of the RI values on particle size. The RI values derived from measurements of aerosols produced from the combustion of hydrocarbons and diesel cannot be used for BB aerosols.
机译:折射率(RI)是描述气溶胶辐射影响的重要参数。限制气溶胶成分的RI非常重要,因为有关燃烧生物质气溶胶的RI仍然存在很大的不确定性。使用T矩阵理论对白松生物量燃烧(BB)气溶胶在两种不同燃烧和采样条件下的实验测量的消光截面,散射截面和单散射反照率进行了建模。从这些计算中提取出折射率。使用腔衰荡光谱仪测量消光,并使用浊度计测量尺寸选择的气溶胶的散射进行实验测量。 BB气雾剂是通过使用以下方法燃烧白松而获得的:(1)在燃烧鼓中的明火中,使用冲击器将气雾剂收集在蒸馏水中,然后在几天后重新雾化,以及(2)管式炉直接将BB气雾剂引入室内烟雾室,然后直接在其中取样BB气雾剂。在这两种情况下,还收集了过滤器样品,并使用电子显微镜图像获得了T矩阵计算中使用的形态和尺寸信息。从明火收集在过滤器介质上的颗粒的有效半径约为245 nm,而对于管式炉燃烧的颗粒,其有效半径约为76 nm。对于在蒸馏水中收集的样品,RI的实部随着粒径的增加而增加,而虚部则减少。 RI的虚部也明显大于新鲜BB气溶胶样品的报告值。对于在管式炉中产生的颗粒,RI的实部随颗粒尺寸而减小,而虚部则小得多且几乎恒定。 RI对粒度和取样方法敏感,但是在所考虑的范围内(500≤λ≤680nm)没有波长依赖性。对于直径为200 nm,300 nm和400 nm的颗粒,新鲜(白松)生物质燃烧气溶胶的RI值范围为1.33 + i0.008至1.74 + i0.008。这些都在密苏拉实验实验室(FLAME I和II)在消防实验室进行的最新研究中RI值的范围内,实际值在1.55至1.80之间,虚构值在0.01〜0.50之间。部分,用于新鲜的BB气雾剂,直径为200±570 nm。 RI值对粒度的依赖性没有明显的趋势。从碳氢化合物和柴油燃烧产生的气溶胶的测量值得出的RI值不能用于BB气溶胶。

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