Differential capacitance of the double layer at the electrode/ionic liquids interface
The differential capacitance of the electrical double layer at glassy carbon, platinum and gold electrodes immersed in various ionic liquids was measured using impedance spectroscopy. We discuss the influence of temperature, the composition of the ionic liquids and the electrode material on the diff...
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Veröffentlicht in: | Physical chemistry chemical physics : PCCP 2010-10, Vol.12 (39), p.12499-12512 |
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creator | Lockett, Vera Horne, Mike Sedev, Rossen Rodopoulos, Theo Ralston, John |
description | The differential capacitance of the electrical double layer at glassy carbon, platinum and gold electrodes immersed in various ionic liquids was measured using impedance spectroscopy. We discuss the influence of temperature, the composition of the ionic liquids and the electrode material on the differential capacitance/potential curves. For different systems these curves have various overall shapes, but all include several extremes and a common minimum near the open circuit potential. We attribute this minimum to the potential of zero charge (PZC). Significantly, the differential capacitance generally decreases if the applied potential is large and moving away from the PZC. This is attributed to lattice saturation [A. A. Kornyshev,
J. Phys. Chem. B
, 2007,
111
, 5545] effects which result in a thicker double layer. The differential capacitance of the double layer grows and specific adsorption diminishes with increasing temperature. Specific adsorption of both cations and anions influences the shapes of curves close to the PZC. The general shape of differential capacitance/potential does not depend strongly on the identity of the electrode material.
The electrical double layer in ionic liquids is different to that in aqueous electrolyte solutions and the differential capacitances curves in ionic liquids are generally "camel"-shaped on different electrode materials. Curves for glassy carbon and gold in [C
4
mim][Tf
2
N] are shown. |
doi_str_mv | 10.1039/c0cp00170h |
format | Article |
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J. Phys. Chem. B
, 2007,
111
, 5545] effects which result in a thicker double layer. The differential capacitance of the double layer grows and specific adsorption diminishes with increasing temperature. Specific adsorption of both cations and anions influences the shapes of curves close to the PZC. The general shape of differential capacitance/potential does not depend strongly on the identity of the electrode material.
The electrical double layer in ionic liquids is different to that in aqueous electrolyte solutions and the differential capacitances curves in ionic liquids are generally "camel"-shaped on different electrode materials. Curves for glassy carbon and gold in [C
4
mim][Tf
2
N] are shown.</description><identifier>ISSN: 1463-9076</identifier><identifier>EISSN: 1463-9084</identifier><identifier>DOI: 10.1039/c0cp00170h</identifier><identifier>PMID: 20721389</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Carbon - chemistry ; Chemistry ; Dielectric Spectroscopy ; Electric Capacitance ; Electrochemistry ; Electrodes ; Exact sciences and technology ; General and physical chemistry ; Gold - chemistry ; Ionic Liquids - chemistry ; Platinum - chemistry ; Surface physical chemistry ; Temperature</subject><ispartof>Physical chemistry chemical physics : PCCP, 2010-10, Vol.12 (39), p.12499-12512</ispartof><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c430t-3303b76e35e1e6a4e60fc699979b71bc7584dbd20f1674b536bdc6ffe6f2a00d3</citedby><cites>FETCH-LOGICAL-c430t-3303b76e35e1e6a4e60fc699979b71bc7584dbd20f1674b536bdc6ffe6f2a00d3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=23356326$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/20721389$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Lockett, Vera</creatorcontrib><creatorcontrib>Horne, Mike</creatorcontrib><creatorcontrib>Sedev, Rossen</creatorcontrib><creatorcontrib>Rodopoulos, Theo</creatorcontrib><creatorcontrib>Ralston, John</creatorcontrib><title>Differential capacitance of the double layer at the electrode/ionic liquids interface</title><title>Physical chemistry chemical physics : PCCP</title><addtitle>Phys Chem Chem Phys</addtitle><description>The differential capacitance of the electrical double layer at glassy carbon, platinum and gold electrodes immersed in various ionic liquids was measured using impedance spectroscopy. We discuss the influence of temperature, the composition of the ionic liquids and the electrode material on the differential capacitance/potential curves. For different systems these curves have various overall shapes, but all include several extremes and a common minimum near the open circuit potential. We attribute this minimum to the potential of zero charge (PZC). Significantly, the differential capacitance generally decreases if the applied potential is large and moving away from the PZC. This is attributed to lattice saturation [A. A. Kornyshev,
J. Phys. Chem. B
, 2007,
111
, 5545] effects which result in a thicker double layer. The differential capacitance of the double layer grows and specific adsorption diminishes with increasing temperature. Specific adsorption of both cations and anions influences the shapes of curves close to the PZC. The general shape of differential capacitance/potential does not depend strongly on the identity of the electrode material.
The electrical double layer in ionic liquids is different to that in aqueous electrolyte solutions and the differential capacitances curves in ionic liquids are generally "camel"-shaped on different electrode materials. Curves for glassy carbon and gold in [C
4
mim][Tf
2
N] are shown.</description><subject>Carbon - chemistry</subject><subject>Chemistry</subject><subject>Dielectric Spectroscopy</subject><subject>Electric Capacitance</subject><subject>Electrochemistry</subject><subject>Electrodes</subject><subject>Exact sciences and technology</subject><subject>General and physical chemistry</subject><subject>Gold - chemistry</subject><subject>Ionic Liquids - chemistry</subject><subject>Platinum - chemistry</subject><subject>Surface physical chemistry</subject><subject>Temperature</subject><issn>1463-9076</issn><issn>1463-9084</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp90D1PwzAQBmALgWgpLOygMCAkpNBznNjJiMqnVImFzpFjn1UjN0ntZOi_J9DSbkw--R7dnV5CLik8UGDFVIFqAaiA5REZ05SzuIA8Pd7Xgo_IWQhfMKCMslMySkAklOXFmCyerDHose6sdJGSrVS2k7XCqDFRt8RIN33lMHJygz6S3e8fOlSdbzRObVNbFTm77q0Oka079EYqPCcnRrqAF7t3QhYvz5-zt3j-8fo-e5zHKmXQxYwBqwRHliFFLlPkYBQvikIUlaCVElme6konYCgXaZUxXmnFh3u5SSSAZhNyt53b-mbdY-jKlQ0KnZM1Nn0oRcbzJIE0GeT9VirfhODRlK23K-k3JYXyJ8XykOKAr3dj-2qFek__YhvA7Q7IoKQzfkjMhoNjLOMs4YO72Tof1L57WFS22gzm6j_DvgG_NI-x</recordid><startdate>20101021</startdate><enddate>20101021</enddate><creator>Lockett, Vera</creator><creator>Horne, Mike</creator><creator>Sedev, Rossen</creator><creator>Rodopoulos, Theo</creator><creator>Ralston, John</creator><general>Royal Society of Chemistry</general><scope>IQODW</scope><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>20101021</creationdate><title>Differential capacitance of the double layer at the electrode/ionic liquids interface</title><author>Lockett, Vera ; Horne, Mike ; Sedev, Rossen ; Rodopoulos, Theo ; Ralston, John</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c430t-3303b76e35e1e6a4e60fc699979b71bc7584dbd20f1674b536bdc6ffe6f2a00d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Carbon - chemistry</topic><topic>Chemistry</topic><topic>Dielectric Spectroscopy</topic><topic>Electric Capacitance</topic><topic>Electrochemistry</topic><topic>Electrodes</topic><topic>Exact sciences and technology</topic><topic>General and physical chemistry</topic><topic>Gold - chemistry</topic><topic>Ionic Liquids - chemistry</topic><topic>Platinum - chemistry</topic><topic>Surface physical chemistry</topic><topic>Temperature</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lockett, Vera</creatorcontrib><creatorcontrib>Horne, Mike</creatorcontrib><creatorcontrib>Sedev, Rossen</creatorcontrib><creatorcontrib>Rodopoulos, Theo</creatorcontrib><creatorcontrib>Ralston, John</creatorcontrib><collection>Pascal-Francis</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Physical chemistry chemical physics : PCCP</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lockett, Vera</au><au>Horne, Mike</au><au>Sedev, Rossen</au><au>Rodopoulos, Theo</au><au>Ralston, John</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Differential capacitance of the double layer at the electrode/ionic liquids interface</atitle><jtitle>Physical chemistry chemical physics : PCCP</jtitle><addtitle>Phys Chem Chem Phys</addtitle><date>2010-10-21</date><risdate>2010</risdate><volume>12</volume><issue>39</issue><spage>12499</spage><epage>12512</epage><pages>12499-12512</pages><issn>1463-9076</issn><eissn>1463-9084</eissn><abstract>The differential capacitance of the electrical double layer at glassy carbon, platinum and gold electrodes immersed in various ionic liquids was measured using impedance spectroscopy. We discuss the influence of temperature, the composition of the ionic liquids and the electrode material on the differential capacitance/potential curves. For different systems these curves have various overall shapes, but all include several extremes and a common minimum near the open circuit potential. We attribute this minimum to the potential of zero charge (PZC). Significantly, the differential capacitance generally decreases if the applied potential is large and moving away from the PZC. This is attributed to lattice saturation [A. A. Kornyshev,
J. Phys. Chem. B
, 2007,
111
, 5545] effects which result in a thicker double layer. The differential capacitance of the double layer grows and specific adsorption diminishes with increasing temperature. Specific adsorption of both cations and anions influences the shapes of curves close to the PZC. The general shape of differential capacitance/potential does not depend strongly on the identity of the electrode material.
The electrical double layer in ionic liquids is different to that in aqueous electrolyte solutions and the differential capacitances curves in ionic liquids are generally "camel"-shaped on different electrode materials. Curves for glassy carbon and gold in [C
4
mim][Tf
2
N] are shown.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><pmid>20721389</pmid><doi>10.1039/c0cp00170h</doi><tpages>14</tpages></addata></record> |
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subjects | Carbon - chemistry Chemistry Dielectric Spectroscopy Electric Capacitance Electrochemistry Electrodes Exact sciences and technology General and physical chemistry Gold - chemistry Ionic Liquids - chemistry Platinum - chemistry Surface physical chemistry Temperature |
title | Differential capacitance of the double layer at the electrode/ionic liquids interface |
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