Evaluation and origins of the difference between double-layer capacitance behaviour at Au-metal and oxidized Au surfaces
In studies of processes at oxidized compared with unoxidized electrode surfaces by transient methods corrections for double-layer charging are usually required and have often been made by extrapolation of double-layer capacitance ( C dl) data for the metallic surface, e.g. at Au or Pt, into the pote...
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description | In studies of processes at oxidized compared with unoxidized electrode surfaces by transient methods corrections for double-layer charging are usually required and have often been made by extrapolation of double-layer capacitance (
C
dl) data for the metallic surface, e.g. at Au or Pt, into the potential region of oxide-film formation. Voltammetry and impedance spectroscopy provide direct information on
C
dl values determined at unoxidized, i.e. metallic, Au surfaces compared with those of anodic oxide films generated potentiostatically to various extents that are stable in time, and characterized by reductive linear-sweep voltammetry.
C
dl is derived from constant-phase element (CPE) values and the CPE parameter,
ϕ, which is near unity for most conditions. At
oxidized Au surfaces
C
dl depends on potential for various extents of oxide formation; it increases from 15 (±1) μF
cm
−2 at 1.75
V (RHE) to 25 (±1) μF
cm
−2 at 1.45
V (RHE) and is independent of added Cl
− or Br
− for concentrations 0–10
−3
M of both anions, while, at
unoxidized Au electrodes in the absence of halide anions,
C
dl has a maximum value of 60 (±2) μF
cm
−2 at 0.80
V (RHE) and is now dependent on concentration of added Cl
− or Br
− ion. These major differences of
C
dl for the oxidized and unoxidized Au surfaces indicate that double-layer charging corrections cannot be made simply by extrapolation of
C
dl data for unoxidized Au metal surfaces into the potential region for oxide formation. |
doi_str_mv | 10.1016/j.electacta.2003.12.009 |
format | Article |
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C
dl) data for the metallic surface, e.g. at Au or Pt, into the potential region of oxide-film formation. Voltammetry and impedance spectroscopy provide direct information on
C
dl values determined at unoxidized, i.e. metallic, Au surfaces compared with those of anodic oxide films generated potentiostatically to various extents that are stable in time, and characterized by reductive linear-sweep voltammetry.
C
dl is derived from constant-phase element (CPE) values and the CPE parameter,
ϕ, which is near unity for most conditions. At
oxidized Au surfaces
C
dl depends on potential for various extents of oxide formation; it increases from 15 (±1) μF
cm
−2 at 1.75
V (RHE) to 25 (±1) μF
cm
−2 at 1.45
V (RHE) and is independent of added Cl
− or Br
− for concentrations 0–10
−3
M of both anions, while, at
unoxidized Au electrodes in the absence of halide anions,
C
dl has a maximum value of 60 (±2) μF
cm
−2 at 0.80
V (RHE) and is now dependent on concentration of added Cl
− or Br
− ion. These major differences of
C
dl for the oxidized and unoxidized Au surfaces indicate that double-layer charging corrections cannot be made simply by extrapolation of
C
dl data for unoxidized Au metal surfaces into the potential region for oxide formation.</description><identifier>ISSN: 0013-4686</identifier><identifier>EISSN: 1873-3859</identifier><identifier>DOI: 10.1016/j.electacta.2003.12.009</identifier><identifier>CODEN: ELCAAV</identifier><language>eng</language><publisher>Oxford: Elsevier Ltd</publisher><subject>Au electrode ; Au oxide formation ; Bromide ; Chemistry ; Chloride ; Electrochemistry ; Exact sciences and technology ; General and physical chemistry ; Impedance ; Miscellaneous ; Perchloric acid ; Study of interfaces</subject><ispartof>Electrochimica acta, 2004-04, Vol.49 (11), p.1775-1788</ispartof><rights>2004 Elsevier Science Ltd</rights><rights>2004 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c374t-fb5d82b2294170393c740876563a52caf556768d5ae0e1a41b642f6f61689543</citedby><cites>FETCH-LOGICAL-c374t-fb5d82b2294170393c740876563a52caf556768d5ae0e1a41b642f6f61689543</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.electacta.2003.12.009$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=15511308$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Germain, Patrick S.</creatorcontrib><creatorcontrib>Pell, Wendy G.</creatorcontrib><creatorcontrib>Conway, Brian E.</creatorcontrib><title>Evaluation and origins of the difference between double-layer capacitance behaviour at Au-metal and oxidized Au surfaces</title><title>Electrochimica acta</title><description>In studies of processes at oxidized compared with unoxidized electrode surfaces by transient methods corrections for double-layer charging are usually required and have often been made by extrapolation of double-layer capacitance (
C
dl) data for the metallic surface, e.g. at Au or Pt, into the potential region of oxide-film formation. Voltammetry and impedance spectroscopy provide direct information on
C
dl values determined at unoxidized, i.e. metallic, Au surfaces compared with those of anodic oxide films generated potentiostatically to various extents that are stable in time, and characterized by reductive linear-sweep voltammetry.
C
dl is derived from constant-phase element (CPE) values and the CPE parameter,
ϕ, which is near unity for most conditions. At
oxidized Au surfaces
C
dl depends on potential for various extents of oxide formation; it increases from 15 (±1) μF
cm
−2 at 1.75
V (RHE) to 25 (±1) μF
cm
−2 at 1.45
V (RHE) and is independent of added Cl
− or Br
− for concentrations 0–10
−3
M of both anions, while, at
unoxidized Au electrodes in the absence of halide anions,
C
dl has a maximum value of 60 (±2) μF
cm
−2 at 0.80
V (RHE) and is now dependent on concentration of added Cl
− or Br
− ion. These major differences of
C
dl for the oxidized and unoxidized Au surfaces indicate that double-layer charging corrections cannot be made simply by extrapolation of
C
dl data for unoxidized Au metal surfaces into the potential region for oxide formation.</description><subject>Au electrode</subject><subject>Au oxide formation</subject><subject>Bromide</subject><subject>Chemistry</subject><subject>Chloride</subject><subject>Electrochemistry</subject><subject>Exact sciences and technology</subject><subject>General and physical chemistry</subject><subject>Impedance</subject><subject>Miscellaneous</subject><subject>Perchloric acid</subject><subject>Study of interfaces</subject><issn>0013-4686</issn><issn>1873-3859</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNqFkEuLFDEQx4MoOI5-BnPRW7d5dJLu47CsD1jwsvdQnVTcDD2dMeked_30ZuhFj0JBQfF_UD9C3nPWcsb1p2OLE7oF6rSCMdly0TI2vCA73hvZyF4NL8mOMS6bTvf6NXlTypExZrRhO_J4e4FphSWmmcLsacrxR5wLTYEuD0h9DAEzzg7piMsvxJn6tI4TNhM8YaYOzuDiApvgAS4xrZnCQg9rc8IFpi30Mfr4G3290rLmAA7LW_IqwFTw3fPek_vPt_c3X5u771--3RzuGidNtzRhVL4XoxBDxw2Tg3SmY73RSktQwkFQShvdewXIkEPHR92JoIPmuh9UJ_fk4xZ7zunnimWxp1gcThPMmNZiRd8Z2dXcPTGb0OVUSsZgzzmeID9ZzuwVtD3av6DtFbTlwlbQ1fnhuQKKgynkSiOWf3alOJesr7rDpsP67iVitsXFK1ofc821PsX_dv0BFDqYyA</recordid><startdate>20040430</startdate><enddate>20040430</enddate><creator>Germain, Patrick S.</creator><creator>Pell, Wendy G.</creator><creator>Conway, Brian E.</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>20040430</creationdate><title>Evaluation and origins of the difference between double-layer capacitance behaviour at Au-metal and oxidized Au surfaces</title><author>Germain, Patrick S. ; Pell, Wendy G. ; Conway, Brian E.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c374t-fb5d82b2294170393c740876563a52caf556768d5ae0e1a41b642f6f61689543</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><topic>Au electrode</topic><topic>Au oxide formation</topic><topic>Bromide</topic><topic>Chemistry</topic><topic>Chloride</topic><topic>Electrochemistry</topic><topic>Exact sciences and technology</topic><topic>General and physical chemistry</topic><topic>Impedance</topic><topic>Miscellaneous</topic><topic>Perchloric acid</topic><topic>Study of interfaces</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Germain, Patrick S.</creatorcontrib><creatorcontrib>Pell, Wendy G.</creatorcontrib><creatorcontrib>Conway, Brian E.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Electrochimica acta</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Germain, Patrick S.</au><au>Pell, Wendy G.</au><au>Conway, Brian E.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Evaluation and origins of the difference between double-layer capacitance behaviour at Au-metal and oxidized Au surfaces</atitle><jtitle>Electrochimica acta</jtitle><date>2004-04-30</date><risdate>2004</risdate><volume>49</volume><issue>11</issue><spage>1775</spage><epage>1788</epage><pages>1775-1788</pages><issn>0013-4686</issn><eissn>1873-3859</eissn><coden>ELCAAV</coden><abstract>In studies of processes at oxidized compared with unoxidized electrode surfaces by transient methods corrections for double-layer charging are usually required and have often been made by extrapolation of double-layer capacitance (
C
dl) data for the metallic surface, e.g. at Au or Pt, into the potential region of oxide-film formation. Voltammetry and impedance spectroscopy provide direct information on
C
dl values determined at unoxidized, i.e. metallic, Au surfaces compared with those of anodic oxide films generated potentiostatically to various extents that are stable in time, and characterized by reductive linear-sweep voltammetry.
C
dl is derived from constant-phase element (CPE) values and the CPE parameter,
ϕ, which is near unity for most conditions. At
oxidized Au surfaces
C
dl depends on potential for various extents of oxide formation; it increases from 15 (±1) μF
cm
−2 at 1.75
V (RHE) to 25 (±1) μF
cm
−2 at 1.45
V (RHE) and is independent of added Cl
− or Br
− for concentrations 0–10
−3
M of both anions, while, at
unoxidized Au electrodes in the absence of halide anions,
C
dl has a maximum value of 60 (±2) μF
cm
−2 at 0.80
V (RHE) and is now dependent on concentration of added Cl
− or Br
− ion. These major differences of
C
dl for the oxidized and unoxidized Au surfaces indicate that double-layer charging corrections cannot be made simply by extrapolation of
C
dl data for unoxidized Au metal surfaces into the potential region for oxide formation.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.electacta.2003.12.009</doi><tpages>14</tpages></addata></record> |
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subjects | Au electrode Au oxide formation Bromide Chemistry Chloride Electrochemistry Exact sciences and technology General and physical chemistry Impedance Miscellaneous Perchloric acid Study of interfaces |
title | Evaluation and origins of the difference between double-layer capacitance behaviour at Au-metal and oxidized Au surfaces |
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