{"id":46,"date":"2023-08-23T20:46:28","date_gmt":"2023-08-23T20:46:28","guid":{"rendered":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/chapter\/equilibrium-fractionation\/"},"modified":"2024-01-11T16:25:08","modified_gmt":"2024-01-11T16:25:08","slug":"equilibrium-fractionation","status":"publish","type":"chapter","link":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/chapter\/equilibrium-fractionation\/","title":{"raw":"4.2 Equilibrium Fractionation","rendered":"4.2 Equilibrium Fractionation"},"content":{"raw":"<div class=\"equilibrium-fractionation\">\r\n<p class=\"import-Normal\">If chemical, physical or exchange reactions are allowed to run to completion, then there will be a fixed isotope difference between the source and receptor reservoirs, at a given temperature. Temperature plays an important role in fractionation. The higher the temperature, the less the degree of fractionation (Figure\u00a07). Once equilibrium is reached, reactions will continue, but backward and forward reactions will occur at an equal rate, with no net effect on isotopic composition of either reservoir. For example, at a given temperature, there is a fixed difference between the <sup>18<\/sup>O\/<sup>16<\/sup>O ratio in H<sub>2<\/sub>O<sub>(l)<\/sub> and H<sub>2<\/sub>O<sub>(<\/sub><sub>v<\/sub><sub>)<\/sub> in equilibrium with each other. In this situation, the kinetic effects of reaction rate are not important, and it is the relative preference for a heavier or lighter isotope within a chemical bond that determines which isotopes are located where, with heavier isotopes favored in bond positions with higher strength. To continue the above example, the hydrogen bonds between water molecules are stronger between H<sub>2<\/sub><sup>18<\/sup>O--H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O than H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O--H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O, and so evaporation will preferentially select for H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O in the vapor mass, resulting in the H<sub>2<\/sub>O<sub>(v)<\/sub> having lower values for <sup>18<\/sup>O\/<sup>16<\/sup>O than the H<sub>2<\/sub>O<sub>(l)<\/sub>.<\/p>\r\n<p class=\"import-Normal\"><img class=\"aligncenter\" src=\"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-content\/uploads\/sites\/33\/2023\/08\/image8.png\" alt=\"image\" width=\"434.437690288714px\" height=\"198.814908136483px\" \/><\/p>\r\n<p class=\"figcaption-text\"><strong>Figure <\/strong><strong>7<\/strong><strong>\u00a0<\/strong><strong>-<\/strong><strong>\u00a0<\/strong>Temperature dependence of fractionation. Graph a) shows the fractionation factor decreasing with rising temperature, and b) shows the difference in isotopic composition between a water source and its evaporated moisture becoming less at higher temperatures, assuming equilibrium conditions.<\/p>\r\n\r\n<\/div>","rendered":"<div class=\"equilibrium-fractionation\">\n<p class=\"import-Normal\">If chemical, physical or exchange reactions are allowed to run to completion, then there will be a fixed isotope difference between the source and receptor reservoirs, at a given temperature. Temperature plays an important role in fractionation. The higher the temperature, the less the degree of fractionation (Figure\u00a07). Once equilibrium is reached, reactions will continue, but backward and forward reactions will occur at an equal rate, with no net effect on isotopic composition of either reservoir. For example, at a given temperature, there is a fixed difference between the <sup>18<\/sup>O\/<sup>16<\/sup>O ratio in H<sub>2<\/sub>O<sub>(l)<\/sub> and H<sub>2<\/sub>O<sub>(<\/sub><sub>v<\/sub><sub>)<\/sub> in equilibrium with each other. In this situation, the kinetic effects of reaction rate are not important, and it is the relative preference for a heavier or lighter isotope within a chemical bond that determines which isotopes are located where, with heavier isotopes favored in bond positions with higher strength. To continue the above example, the hydrogen bonds between water molecules are stronger between H<sub>2<\/sub><sup>18<\/sup>O&#8211;H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O than H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O&#8211;H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O, and so evaporation will preferentially select for H<sub>2<\/sub><sup>1<\/sup><sup>6<\/sup>O in the vapor mass, resulting in the H<sub>2<\/sub>O<sub>(v)<\/sub> having lower values for <sup>18<\/sup>O\/<sup>16<\/sup>O than the H<sub>2<\/sub>O<sub>(l)<\/sub>.<\/p>\n<p class=\"import-Normal\"><img decoding=\"async\" class=\"aligncenter\" src=\"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-content\/uploads\/sites\/33\/2023\/08\/image8.png\" alt=\"image\" width=\"434.437690288714px\" height=\"198.814908136483px\" \/><\/p>\n<p class=\"figcaption-text\"><strong>Figure <\/strong><strong>7<\/strong><strong>\u00a0<\/strong><strong>&#8211;<\/strong><strong>\u00a0<\/strong>Temperature dependence of fractionation. Graph a) shows the fractionation factor decreasing with rising temperature, and b) shows the difference in isotopic composition between a water source and its evaporated moisture becoming less at higher temperatures, assuming equilibrium conditions.<\/p>\n<\/div>\n","protected":false},"author":4,"menu_order":4,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-46","chapter","type-chapter","status-publish","hentry"],"part":162,"_links":{"self":[{"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/pressbooks\/v2\/chapters\/46","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/wp\/v2\/users\/4"}],"version-history":[{"count":4,"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/pressbooks\/v2\/chapters\/46\/revisions"}],"predecessor-version":[{"id":419,"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/pressbooks\/v2\/chapters\/46\/revisions\/419"}],"part":[{"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/pressbooks\/v2\/parts\/162"}],"metadata":[{"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/pressbooks\/v2\/chapters\/46\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/wp\/v2\/media?parent=46"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/pressbooks\/v2\/chapter-type?post=46"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/wp\/v2\/contributor?post=46"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/books.gw-project.org\/stable-isotope-hydrology\/wp-json\/wp\/v2\/license?post=46"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}