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研究生:林秀姿
研究生(外文):Lin, 秀姿
論文名稱:台灣地區大氣氣膠特性之研究-氣膠散光係數粒徑分布
論文名稱(外文):Characteristics of atmospheric Aerosols in Taiwan- aerosol light-scattering coefficient aerosol size distribution
指導教授:李崇德李崇德引用關係
指導教授(外文):C.-T. Lee
學位類別:碩士
校院名稱:國立中央大學
系所名稱:環境工程學系
學門:工程學門
學類:環境工程學類
論文種類:學術論文
論文出版年:1998
畢業學年度:86
語文別:中文
論文頁數:91
中文關鍵詞:散光係數氣膠粒徑分布氣膠形狀電移動度粒徑
外文關鍵詞:Light-scattering coefficientaerosol size distributionshape of aerosolmobolity diameter
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氣膠對於太陽輻射的散射的能力於全球溫室效應的評估具有重大的影響
。影響散光係數(ssp)的原因很多,其中氣膠粒徑分布為主要的影響因素
之一,雖然散光係數是所有粒徑氣膠的整體表現,然而找出影響散光係數
優勢粒徑將有助於空氣污染防治策略的擬定。本研究以掃描式移動度粒徑
分析儀(SMPS, TSI Model 3934)及積分散光儀(TSIModel 3563)分別量測
不同形狀氣膠散光係數粒徑分布及實測大氣氣膠散光係數粒徑分布。 在
實驗室研究結果顯示,相同移動度粒徑的圓球、短柱與長柱狀氣膠,其散
光係數隨著長寬比的增加而增大,長寬比越大的氣膠背散光係數越小;在
光源方面,波長越短散光係數越大;圓球、短柱與長柱氣膠的散光效率差
異不大。 利用相同實驗系統,在位於郊區的中央大學及台北縣三重市的
環保署空氣品質監測站實測大氣氣膠散光係數粒徑分布,量測結果郊區氣
膠散光係數在0.06km-1~0.14km-1,散光係數粒徑分布呈單尖峰分布,尖
峰值位於粒徑0.5mm,三重地區氣膠散光係數在0.08km-1~ 0.36km-1,散
光係數粒徑分布呈雙尖峰分布,尖峰值分別位於粒徑0.45mm及0.65mm。研
究結果顯示,中央大學及三重地區理論散光係數(ssp,c)約佔實測粒徑散
光係數和(Sssp)的89%及82%,中央大學實測粒徑散光係數和約佔實測散光
係數的80%,三重地區實測粒徑散光係數和約佔實測散光係數的81%。

The light scattering of atmospheric aerosols are important in
radiative forcing in global warming. Among factors affecting
aerosol light-scattering coefficient (ssp), aerosol size
distribution has been known to be a major one. Although ssp is
an integrating effect from all sizes of aerosols, a revelation
of significant sizes in determining ssp is crucial in
evaluating the control measures for atmospheric visibility. In
the present study, a system consists of a scanning mobility
particle sizer (SMPS, TSI Model 3934) and an integrating
nephelometer (TSI Model 3563) was set up to assess shape
effects on ssp size distribution and measure ssp size
distribution. For the same mobility diameter, ssp is shown
increased with an increasing ratio of long-to-short axis among
sphere, short prism, and long prism. Meanwhile, aerosol back-
scattering coefficient is decreased for an increasing ratio of
long-to-short axis. The ssp size distribution was measured
both at the campus of National Central University (NCU, in a
suburban area) and at Sun-chun air quality monitoring station
(on a traffic laden road). The results at NCU site showed a
uni-modal ssp size distribution with a peak diameter at 0.5mm
and the ssp in the range of 0.06~0.14Km-1. In contrast, Sun-
chun site showed a bi-modal ssp size distribution with peak
diameters at 0.45mm and 0.65 mm, individually, and the ssp in
the range of 0.08~0.36Km-1. In the present study, a
theoretical ssp size distribution is calculated from Mie theory
and the measured aerosol size distribution. For a comparison,
the ratio of the sum from theoretical ssp size distribution to
that from measured ssp size is 89% and 82% at NCU site and
Sun-chun site, individually. Meanwhile, the ratio of
theoretical ssp to the sum from theoretical ssp size
distribution is 80% and 81% at NCU site and Sun-Chun site
,individually.

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