Ion parking in native mass spectrometry
A forced, damped harmonic oscillator model for gas-phase ion parking using single-frequency resonance excitation is described and applied to high-mass ions of relevance to native mass spectrometry. Experimental data are provided to illustrate key findings revealed by the modelling. These include: (i...
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Veröffentlicht in: | Analyst (London) 2024-05, Vol.149 (1), p.2966-2977 |
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creator | Pizzala, Nicolas J Bhanot, Jay S Carrick, Ian J Dziekonski, Eric T McLuckey, Scott A |
description | A forced, damped harmonic oscillator model for gas-phase ion parking using single-frequency resonance excitation is described and applied to high-mass ions of relevance to native mass spectrometry. Experimental data are provided to illustrate key findings revealed by the modelling. These include: (i) ion secular frequency spacings between adjacent charge states of a given protein are essentially constant and decrease with the mass of the protein (ii) the mechanism for ion parking of high mass ions is the separation of the ion clouds of the oppositely-charged ions with much less influence from an increase in the relative ion velocity due to resonance excitation, (iii) the size of the parked ion cloud ultimately limits ion parking at high
m
/
z
ratio, and (iv) the extent of ion parking of off-target ions is highly sensitive to the bath gas pressure in the ion trap. The model is applied to ions of 17 kDa, 467 kDa, and 2 MDa while experimental data are also provided for ions of horse skeletal muscle myoglobin ( 17 kDa) and β-galactosidase ( 467 kDa). The model predicts and data show that it is possible to effect ion parking on a 17 kDa protein to the 1
+
charge state under trapping conditions that are readily accessible with commercially available ion traps. It is also possible to park β-galactosidase efficiently to a roughly equivalent
m
/
z
ratio (
i.e.
, the 26
+
charge state) under the same trapping conditions. However, as charge states decrease, analyte ion cloud sizes become too large to allow for efficient ion trapping. The model allows for a semi-quantitative prediction of ion trapping performance as a function of ion trapping, resonance excitation, and pressure conditions.
It is possible to inhibit the rates of ion-ion reactions involving high mass ions
via
the selective separation of reactant ion clouds. A comprehensive model for predicting conditions for successful ion parking with illustrative data are provided. |
doi_str_mv | 10.1039/d4an00242c |
format | Article |
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m
/
z
ratio, and (iv) the extent of ion parking of off-target ions is highly sensitive to the bath gas pressure in the ion trap. The model is applied to ions of 17 kDa, 467 kDa, and 2 MDa while experimental data are also provided for ions of horse skeletal muscle myoglobin ( 17 kDa) and β-galactosidase ( 467 kDa). The model predicts and data show that it is possible to effect ion parking on a 17 kDa protein to the 1
+
charge state under trapping conditions that are readily accessible with commercially available ion traps. It is also possible to park β-galactosidase efficiently to a roughly equivalent
m
/
z
ratio (
i.e.
, the 26
+
charge state) under the same trapping conditions. However, as charge states decrease, analyte ion cloud sizes become too large to allow for efficient ion trapping. The model allows for a semi-quantitative prediction of ion trapping performance as a function of ion trapping, resonance excitation, and pressure conditions.
It is possible to inhibit the rates of ion-ion reactions involving high mass ions
via
the selective separation of reactant ion clouds. A comprehensive model for predicting conditions for successful ion parking with illustrative data are provided.</description><identifier>ISSN: 0003-2654</identifier><identifier>EISSN: 1364-5528</identifier><identifier>DOI: 10.1039/d4an00242c</identifier><identifier>PMID: 38600834</identifier><language>eng</language><publisher>England: Royal Society of Chemistry</publisher><subject>Chemistry ; Excitation ; Galactosidase ; Gas pressure ; Harmonic oscillators ; Ion traps (instrumentation) ; Ion velocity ; Ions ; Mass spectrometry ; Myoglobins ; Parking ; Proteins ; Resonance ; Scientific imaging</subject><ispartof>Analyst (London), 2024-05, Vol.149 (1), p.2966-2977</ispartof><rights>Copyright Royal Society of Chemistry 2024</rights><rights>This journal is © The Royal Society of Chemistry 2024 The Royal Society of Chemistry</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c429t-3bb437e10df70dff7dbe049549ae19febc32bd022e0bf1576885e27518eb3163</citedby><cites>FETCH-LOGICAL-c429t-3bb437e10df70dff7dbe049549ae19febc32bd022e0bf1576885e27518eb3163</cites><orcidid>0000-0001-6473-9611 ; 0000-0002-1648-5570</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,778,782,883,2820,2821,27911,27912</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/38600834$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Pizzala, Nicolas J</creatorcontrib><creatorcontrib>Bhanot, Jay S</creatorcontrib><creatorcontrib>Carrick, Ian J</creatorcontrib><creatorcontrib>Dziekonski, Eric T</creatorcontrib><creatorcontrib>McLuckey, Scott A</creatorcontrib><title>Ion parking in native mass spectrometry</title><title>Analyst (London)</title><addtitle>Analyst</addtitle><description>A forced, damped harmonic oscillator model for gas-phase ion parking using single-frequency resonance excitation is described and applied to high-mass ions of relevance to native mass spectrometry. Experimental data are provided to illustrate key findings revealed by the modelling. These include: (i) ion secular frequency spacings between adjacent charge states of a given protein are essentially constant and decrease with the mass of the protein (ii) the mechanism for ion parking of high mass ions is the separation of the ion clouds of the oppositely-charged ions with much less influence from an increase in the relative ion velocity due to resonance excitation, (iii) the size of the parked ion cloud ultimately limits ion parking at high
m
/
z
ratio, and (iv) the extent of ion parking of off-target ions is highly sensitive to the bath gas pressure in the ion trap. The model is applied to ions of 17 kDa, 467 kDa, and 2 MDa while experimental data are also provided for ions of horse skeletal muscle myoglobin ( 17 kDa) and β-galactosidase ( 467 kDa). The model predicts and data show that it is possible to effect ion parking on a 17 kDa protein to the 1
+
charge state under trapping conditions that are readily accessible with commercially available ion traps. It is also possible to park β-galactosidase efficiently to a roughly equivalent
m
/
z
ratio (
i.e.
, the 26
+
charge state) under the same trapping conditions. However, as charge states decrease, analyte ion cloud sizes become too large to allow for efficient ion trapping. The model allows for a semi-quantitative prediction of ion trapping performance as a function of ion trapping, resonance excitation, and pressure conditions.
It is possible to inhibit the rates of ion-ion reactions involving high mass ions
via
the selective separation of reactant ion clouds. A comprehensive model for predicting conditions for successful ion parking with illustrative data are provided.</description><subject>Chemistry</subject><subject>Excitation</subject><subject>Galactosidase</subject><subject>Gas pressure</subject><subject>Harmonic oscillators</subject><subject>Ion traps (instrumentation)</subject><subject>Ion velocity</subject><subject>Ions</subject><subject>Mass spectrometry</subject><subject>Myoglobins</subject><subject>Parking</subject><subject>Proteins</subject><subject>Resonance</subject><subject>Scientific imaging</subject><issn>0003-2654</issn><issn>1364-5528</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNpdkctLw0AQxhdRbK1evCsBD4oQnX3lcZJSX4Wil96XTTKpqcmm7iaF_vemttbHYRiG78fHzDeEnFK4ocDj20xoA8AES_dIn_JA-FKyaJ_0AYD7LJCiR46cm3cjBQmHpMejACDiok8ux7XxFtq-F2bmFcYzuimW6FXaOc8tMG1sXWFjV8fkINelw5NtH5Dp48N09OxPXp_Go-HETwWLG58nieAhUsjysKs8zBIEEUsRa6RxjknKWZIBYwhJTmUYRJFEFkoaYcJpwAfkbmO7aJMKsxRNY3WpFraotF2pWhfqr2KKNzWrl4pSiGLJWOdwtXWw9UeLrlFV4VIsS22wbp3iwEMeiyBYoxf_0HndWtOd11GSxywKKO-o6w2V2to5i_luGwpqnb-6F8OXr_xHHXz-e_8d-h14B5xtAOvSnfrzQP4J0HyJDw</recordid><startdate>20240513</startdate><enddate>20240513</enddate><creator>Pizzala, Nicolas J</creator><creator>Bhanot, Jay S</creator><creator>Carrick, Ian J</creator><creator>Dziekonski, Eric T</creator><creator>McLuckey, Scott A</creator><general>Royal Society of Chemistry</general><general>The Royal Society of Chemistry</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7X8</scope><scope>5PM</scope><orcidid>https://orcid.org/0000-0001-6473-9611</orcidid><orcidid>https://orcid.org/0000-0002-1648-5570</orcidid></search><sort><creationdate>20240513</creationdate><title>Ion parking in native mass spectrometry</title><author>Pizzala, Nicolas J ; Bhanot, Jay S ; Carrick, Ian J ; Dziekonski, Eric T ; McLuckey, Scott A</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c429t-3bb437e10df70dff7dbe049549ae19febc32bd022e0bf1576885e27518eb3163</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Chemistry</topic><topic>Excitation</topic><topic>Galactosidase</topic><topic>Gas pressure</topic><topic>Harmonic oscillators</topic><topic>Ion traps (instrumentation)</topic><topic>Ion velocity</topic><topic>Ions</topic><topic>Mass spectrometry</topic><topic>Myoglobins</topic><topic>Parking</topic><topic>Proteins</topic><topic>Resonance</topic><topic>Scientific imaging</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Pizzala, Nicolas J</creatorcontrib><creatorcontrib>Bhanot, Jay S</creatorcontrib><creatorcontrib>Carrick, Ian J</creatorcontrib><creatorcontrib>Dziekonski, Eric T</creatorcontrib><creatorcontrib>McLuckey, Scott A</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Analyst (London)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Pizzala, Nicolas J</au><au>Bhanot, Jay S</au><au>Carrick, Ian J</au><au>Dziekonski, Eric T</au><au>McLuckey, Scott A</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Ion parking in native mass spectrometry</atitle><jtitle>Analyst (London)</jtitle><addtitle>Analyst</addtitle><date>2024-05-13</date><risdate>2024</risdate><volume>149</volume><issue>1</issue><spage>2966</spage><epage>2977</epage><pages>2966-2977</pages><issn>0003-2654</issn><eissn>1364-5528</eissn><abstract>A forced, damped harmonic oscillator model for gas-phase ion parking using single-frequency resonance excitation is described and applied to high-mass ions of relevance to native mass spectrometry. Experimental data are provided to illustrate key findings revealed by the modelling. These include: (i) ion secular frequency spacings between adjacent charge states of a given protein are essentially constant and decrease with the mass of the protein (ii) the mechanism for ion parking of high mass ions is the separation of the ion clouds of the oppositely-charged ions with much less influence from an increase in the relative ion velocity due to resonance excitation, (iii) the size of the parked ion cloud ultimately limits ion parking at high
m
/
z
ratio, and (iv) the extent of ion parking of off-target ions is highly sensitive to the bath gas pressure in the ion trap. The model is applied to ions of 17 kDa, 467 kDa, and 2 MDa while experimental data are also provided for ions of horse skeletal muscle myoglobin ( 17 kDa) and β-galactosidase ( 467 kDa). The model predicts and data show that it is possible to effect ion parking on a 17 kDa protein to the 1
+
charge state under trapping conditions that are readily accessible with commercially available ion traps. It is also possible to park β-galactosidase efficiently to a roughly equivalent
m
/
z
ratio (
i.e.
, the 26
+
charge state) under the same trapping conditions. However, as charge states decrease, analyte ion cloud sizes become too large to allow for efficient ion trapping. The model allows for a semi-quantitative prediction of ion trapping performance as a function of ion trapping, resonance excitation, and pressure conditions.
It is possible to inhibit the rates of ion-ion reactions involving high mass ions
via
the selective separation of reactant ion clouds. A comprehensive model for predicting conditions for successful ion parking with illustrative data are provided.</abstract><cop>England</cop><pub>Royal Society of Chemistry</pub><pmid>38600834</pmid><doi>10.1039/d4an00242c</doi><tpages>12</tpages><orcidid>https://orcid.org/0000-0001-6473-9611</orcidid><orcidid>https://orcid.org/0000-0002-1648-5570</orcidid><oa>free_for_read</oa></addata></record> |
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source | Royal Society of Chemistry Journals Archive (1841-2007); Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
subjects | Chemistry Excitation Galactosidase Gas pressure Harmonic oscillators Ion traps (instrumentation) Ion velocity Ions Mass spectrometry Myoglobins Parking Proteins Resonance Scientific imaging |
title | Ion parking in native mass spectrometry |
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