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→‎Faasejlëijshjeweesh: Zemmlesch fäädesch övvosaz
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== Faasejlëijshjeweesh ==
De kinneetėshe Ënnëjii eß op de [[Mollekühl]] nit ejaal fodëëijlt, se wääßelt zohfällėsh.
{{Övversäzze}}
Dat bedügk zem Bëijshpell dat, aan de Ovverfläsh fon_enne Fößßeshkëijt, doh könnd_ėmmer mohl e ëijnzel Mollkühl med_jenooch kinneetėshe Ënnëjii optrëdde, dat dat en de Jaaßfaaß erövver höppe könnt. Jeno_esu_joot kann_e ëijnzel Jahßmollekühl winnėsh jenooch kinneetėsh Ënnëjii han, dat dat sesh met_ä annderre Mollekühle en de flößėje Faaß zosamme donn kann. Dat bedück, dat bëij bëijnah jeede Kombenazjohn fon Drok un Tëmpratuur ongersheedlijje Faase zosamme dohsėnn könne.
The distribution of kinetic energy among molecules is not uniform, and it changes randomly. This means that at, say, the surface of a liquid, there may be an individual molecule with enough kinetic energy to jump into the gas phase. Likewise, individual gas molecules may have low enough kinetic energy to join other molecules in the liquid phase. This phenomenon means that at any given temperature and pressure, multiple phases may co-exist.
 
Förr_e Bëijshpell weet onger de [[Shtanndat_Bedėngonge för Tëmpratuur un Drok]] fon enne Schößel med flößßijem Waßo en drüjje Luvv_enne Aandëijl fodůnnßte, beß dat dä [[aandëijlejje Drok]] fom WaßoJaaß jenou_esu_jrooß eß, wi dä [[Damfdrok (Füssėk)]] fom flößßėje Waßo. Aan dämm Pungk, well saare, en dämm Zohshtannd,_eß di Aanzahl Molleküül, di de zwesche dä Faase wäähßelt, en bėijde Rėshtonge jlisch.
For example, under [[standard conditions for temperature and pressure]], a bowl of liquid water in dry air will evaporate until the [[partial pressure]] of gaseous water equals the [[vapor pressure]] of water. At this point, the rate of molecules leaving and entering the liquid phase becomes the same (due to the increased number of gaseous water molecules available to re-condense). The fact that liquid molecules with above-average kinetic energy have been removed from the bowl results in [[evaporative cooling]]. Similar processes may occur on other types of phase boundaries.
<!-- (due to the increased number of gaseous water molecules available to re-condense)-->
Dat fon dä flößßėjje Mollekül met övver_dorshschnettlijje kinneetėshe Ënnëjii wëllshe uß dä Schößel affjehoue sin, hät doh dämm ëntshprëshend_en [[Fodamfongkällte]] erėnn_jebraat. Äähnlejje Föejäng hät me aan annder Aate fon Faasejrënze och.
 
Em [[Willard Gibbs|Gibbs]] sing [[Gibbs_sėng Faase_Rääjel|Faase_Rääjel]] säz de Aanzahl fon mööshlejje Faase med_esu [[Varrijaable (Füssėk)|Varrijaable]] wi Tëmpratuur un Drok un esu wigger en_t Fohälltnėß, un sääd_onß of e Jlëijshjeweesch optredde kann, oddo optrëdde weed.
[[Willard Gibbs|Gibbs']] [[Gibbs phase rule|phase rule]] relates the number of possible phases, variables such as temperature and pressure, and whether or not an equilibrium will be reached.
 
== Faase'övverjäng ==
Di Sigg heh stamp vun „https://ksh.wikipedia.org/wiki/Faaß_(Füsėk)“.