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化學 1918

氣體在玻璃、雲母與鉑平面上的吸附

歐文·朗繆爾

氣體只在固體上吸附一層分子那麼深——而這單薄的一層,奠定了表面化學。

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In depth · the introduction

當氣體黏到固體上時,它並不會越堆越高——它鋪下恰好一層分子那麼厚的一層,然後就停住了。

核心想法

把一塊乾淨的表面放進氣體裡,總有一部分氣體會黏上去。這早不是新聞。歐文·朗繆爾的洞見,關乎黏上去多少。他論證說,把氣體分子按在固體上的力,短程到只能抓住直接挨著表面的那些分子。疊在第一層之上的第二個分子,幾乎什麼也感覺不到。於是這層黏附物只有一層分子那麼深——一層漆,絕不會有兩層。

從這一幅圖,他得到了一條乾淨的規則。把表面想成一排座位。氣體分子不斷落進空座,落座的分子又不斷起身離開。把氣體壓強往上推,更多座位被坐滿——但只能填到這排座位坐滿為止。被佔座位的比例,沿著一條俐落的曲線走:先快速上升,再在「滿座」處變平。這條曲線就是朗繆爾等溫線,也是表面化學的根基。

它是如何誕生的

朗繆爾是個不尋常的人物:他不是大學教授,而是紐約州斯克內克塔迪奇異研究實驗室裡的一名工業科學家,受雇去弄清燈泡燈絲為何會燒斷。在追究灼熱金屬絲、以及絲上那層薄薄的氣膜如何行事的過程中,他被捲入了一個更深的問題:氣體究竟是怎樣與固體相遇的——而他帶著一個實驗家對極低壓下潔淨測量的執著。

1918 年的論文,正是由此而來。它如此富有成果,以致在 1932 年幫他成為第一位出身工業界、而非大學的諾貝爾化學獎得主。許多表面工作,是他與凱瑟琳·布洛傑特一同完成的——「朗繆爾—布洛傑特膜」之名裡留著她,那正是從這項研究裡直接長出來的;她後來還發明了用於相機鏡頭與眼鏡的無反射玻璃。

它為何重要

幾乎一切有用的事,都發生在表面上:催化劑在它的表面上加速反應,活性炭濾芯在它的表面上截住氣味,感測器靠黏上它表面的東西來探測氣體。在朗繆爾之前,「黏到表面上」是個含糊的概念;在他之後,它成了一個你能預測、能測量、能據以設計的數字。他那條方程,至今仍是化學家弄清一份粉末有多大表面、一種催化劑會如何行事、一個濾芯能容納多少污染物的辦法。

一個可以想像的畫面

想像一個車位數量固定的停車場。車(氣體分子)不斷駛入,也不斷駛離。車流稀少時,幾乎每輛來的車都能找到位子,於是車場大致隨來車的多少同步填滿。可一旦擠起來,新來的車越來越常發現位子全滿、只好開走。車場永遠不會超過「滿」——而關鍵是,你沒法把車疊到車上。這「先一層、然後滿」,正是朗繆爾的表面,而那條填充曲線,就是他的等溫線。

可互動的朗繆爾吸附等溫線:一個滑桿升高氣體壓強,另一個設定氣體黏附得多強;曲線與一格格表面位點先快速填滿、再隨單層飽和而趨於平坦。

它的位置

這是表面化學的誕生,它立足於本館已有的道爾頓、亞佛加厥與路易斯的原子圖景,也立足於吉布斯的平衡思想。引人注目的是,同樣這條 S 形的飽和曲線,五年前就在生物學裡出現過——米氏酶動力學定律,本館也有——因為兩者講的是同一個故事:東西填滿一組固定的位點。朗繆爾的單分子層,後來被 BET 理論疊成多層,而那正是表面積至今的測量之法。

The original document
Original source text
Irving Langmuir · J. Am. Chem. Soc. 40 (1918) 1361–1403 · "The Adsorption of Gases on Plane Surfaces of Glass, Mica and Platinum"
The single-layer postulate
[Editorial summary] Langmuir opens by arguing that the forces holding a gas onto a solid are short-ranged — essentially the same valence forces that bind atoms in molecules, reaching out only about a molecular diameter. From this one premise a sharp conclusion follows: an adsorbed gas film, in most cases, can be only one molecule thick. The surface offers a fixed number of sites, and once a site is occupied the molecule above it lies beyond the reach of the surface's grip.
Adsorption as a dynamic balance
[Editorial summary] He then treats adsorption not as a static coating but as a continuous traffic: gas molecules strike the surface and stick to bare sites at a rate set by the pressure, while adsorbed molecules are forever evaporating back off. Equilibrium is the standstill where the two rates match — not an empty or a full surface, but a steady covered fraction that the molecules constantly turn over.
The isotherm
[Editorial summary] Setting the rate of condensation onto empty sites equal to the rate of evaporation from filled ones yields his isotherm: the fraction θ of the surface covered is bP/(1+bP), where P is the gas pressure and b measures how strongly the gas binds. The curve rises almost linearly at low pressure, bends over, and flattens toward θ = 1 as the single layer fills — the saturation that ordinary 'condensation' pictures could not explain. Langmuir checks this shape against his careful low-pressure measurements on glass, mica and platinum.
Mixtures, dissociation and reaction
[Editorial summary] The paper extends the same bookkeeping to several gases competing for the same sites, to molecules that split into two fragments on adsorbing (each needing a site), and to the way a surface that holds reactants is the stage on which catalysis happens — the seed of what became the Langmuir–Hinshelwood picture of surface reactions.
[ … ]
General Electric Research Laboratory, Schenectady · 1918