Transient electric birefringence of agarose gels. II. Reversing electric fields and comparison with other polymer gels
The transient electric birefringence of low electroendosmosis (LE) agarose gels oriented by pulsed unidirectional electric fields was described in detail in Part I [J. Stellwagen and N. C. Stellwagen (1994), Biopolymers, Vol. 34, p. 187]. Here, the birefringence of LE agarose gels in rapidly reversi...
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description | The transient electric birefringence of low electroendosmosis (LE) agarose gels oriented by pulsed unidirectional electric fields was described in detail in Part I [J. Stellwagen and N. C. Stellwagen (1994), Biopolymers, Vol. 34, p. 187]. Here, the birefringence of LE agarose gels in rapidly reversing electric fields, similar in amplitude and duration to those used for field inversion gel electrophoresis, is reported.
Symmetric reversing electric fields cause the sign of the birefringence of LE agarose gels, and hence the direction of orientation of the agarose fibers, to Oscillate in phase with the applied electric field. Because of long‐lasting memory effects, the alternating sign of the birefringence appears to be due to metastable changes in gel structure induced by the electric field. If the reversing field pulses are equal in amplitude but different in duration, the orientation behavior depends critically on the applied voltage. If E < 7 V/cm, the amplitude of the birefringence gradually decreases with increasing pulse number and becomes unmeasurably small. However, if E > 7 V/cm, the amplitude of the birefringence increase more than 10‐fold after ∼ 20 pulses have been applied to the gel, suggesting that a cooperative change in gel structure has occurred. Because there is no concomitant change birefringence must be due to an increase in the number of agarose fibers and /or fiber bundles orienting in the lectric field, which in turn indicates a cooperatice breakdown of the noncovalent “junction zones” that corss‐link the fibers in to the fgel matrix. The sign of the birefringence of LE agarose gels is always positive after extensive junction zone breakdown, indicating that the agarose fibers and fiber bundles preferentially orient parallel to the lectric field when they are freed from the constraints of the gel matrix.
Three other gel‐forming polymers, high electroendosmosis (HEEO) agarose (a more highly changed agarose), β‐carrageenan (a stereoisomer of agarose), and polyacrylamide (a chemically corss‐linked polymer) were alos studied in unidirectional and rapidly reversing electric fields. The birefringence of HEEO agarose backbone chain. The β‐carrageenan gels exhibit variable orientation behavior in reversing electric fields, suggesting that its internal gel structure is not as tightly interconnected as that of agaroise gels. Both HEEO agarose and β‐carrageenan gels exhibit a large increase in the amplitude of the birefringence with increasing pul |
doi_str_mv | 10.1002/bip.360340914 |
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Symmetric reversing electric fields cause the sign of the birefringence of LE agarose gels, and hence the direction of orientation of the agarose fibers, to Oscillate in phase with the applied electric field. Because of long‐lasting memory effects, the alternating sign of the birefringence appears to be due to metastable changes in gel structure induced by the electric field. If the reversing field pulses are equal in amplitude but different in duration, the orientation behavior depends critically on the applied voltage. If E < 7 V/cm, the amplitude of the birefringence gradually decreases with increasing pulse number and becomes unmeasurably small. However, if E > 7 V/cm, the amplitude of the birefringence increase more than 10‐fold after ∼ 20 pulses have been applied to the gel, suggesting that a cooperative change in gel structure has occurred. Because there is no concomitant change birefringence must be due to an increase in the number of agarose fibers and /or fiber bundles orienting in the lectric field, which in turn indicates a cooperatice breakdown of the noncovalent “junction zones” that corss‐link the fibers in to the fgel matrix. The sign of the birefringence of LE agarose gels is always positive after extensive junction zone breakdown, indicating that the agarose fibers and fiber bundles preferentially orient parallel to the lectric field when they are freed from the constraints of the gel matrix.
Three other gel‐forming polymers, high electroendosmosis (HEEO) agarose (a more highly changed agarose), β‐carrageenan (a stereoisomer of agarose), and polyacrylamide (a chemically corss‐linked polymer) were alos studied in unidirectional and rapidly reversing electric fields. The birefringence of HEEO agarose backbone chain. The β‐carrageenan gels exhibit variable orientation behavior in reversing electric fields, suggesting that its internal gel structure is not as tightly interconnected as that of agaroise gels. Both HEEO agarose and β‐carrageenan gels exhibit a large increase in the amplitude of the birefringence with increasing pulse number when asymmetric reversing pulses > 7 V/cm are applied to the gels, suggesting that junction zone breakdown in a common feature of polysaccharide gels.
Chemically cross‐linked polyacrylamide gels exhibit very small birefringence signals, indicating that very little orientation occurs in pulsed lectric fields. The sign of the birefringence is independent of the polarity of the lectric field, as expected from the Kerr law, and normal orientation behavior is observed in reversing electric fields. Hence, the anomalous change in sign of the birefringence observed for agarose gels in reversing electric fields must be due to the metastable junction zones in the agarose gel matrix, which allow gel fiber rearrangements to occur. © 1994 John Wiley & Sons, Inc.</description><identifier>ISSN: 0006-3525</identifier><identifier>EISSN: 1097-0282</identifier><identifier>DOI: 10.1002/bip.360340914</identifier><identifier>PMID: 7948738</identifier><identifier>CODEN: BIPMAA</identifier><language>eng</language><publisher>Hoboken: Wiley Subscription Services, Inc., A Wiley Company</publisher><subject>Analytical biochemistry: general aspects, technics, instrumentation ; Analytical, structural and metabolic biochemistry ; Biological and medical sciences ; Birefringence ; Carbohydrate Sequence ; Chemical Phenomena ; Chemistry, Physical ; Electromagnetic Fields ; Electrophoresis, Agar Gel - methods ; Fundamental and applied biological sciences. Psychology ; Gels - chemistry ; Molecular Sequence Data ; Polymers - chemistry ; Sepharose - chemistry</subject><ispartof>Biopolymers, 1994-09, Vol.34 (9), p.1259-1273</ispartof><rights>Copyright © 1994 John Wiley & Sons, Inc.</rights><rights>1994 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3184-364f32389b7bfc283f27272701b2f092da980f712deda254000011b1db8c3cdf3</citedby><cites>FETCH-LOGICAL-c3184-364f32389b7bfc283f27272701b2f092da980f712deda254000011b1db8c3cdf3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fbip.360340914$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fbip.360340914$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,776,780,1411,27901,27902,45550,45551</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=4217914$$DView record in Pascal Francis$$Hfree_for_read</backlink><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/7948738$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Stellwagen, John</creatorcontrib><creatorcontrib>Stellwagen, Nancy C.</creatorcontrib><title>Transient electric birefringence of agarose gels. II. Reversing electric fields and comparison with other polymer gels</title><title>Biopolymers</title><addtitle>Biopolymers</addtitle><description>The transient electric birefringence of low electroendosmosis (LE) agarose gels oriented by pulsed unidirectional electric fields was described in detail in Part I [J. Stellwagen and N. C. Stellwagen (1994), Biopolymers, Vol. 34, p. 187]. Here, the birefringence of LE agarose gels in rapidly reversing electric fields, similar in amplitude and duration to those used for field inversion gel electrophoresis, is reported.
Symmetric reversing electric fields cause the sign of the birefringence of LE agarose gels, and hence the direction of orientation of the agarose fibers, to Oscillate in phase with the applied electric field. Because of long‐lasting memory effects, the alternating sign of the birefringence appears to be due to metastable changes in gel structure induced by the electric field. If the reversing field pulses are equal in amplitude but different in duration, the orientation behavior depends critically on the applied voltage. If E < 7 V/cm, the amplitude of the birefringence gradually decreases with increasing pulse number and becomes unmeasurably small. However, if E > 7 V/cm, the amplitude of the birefringence increase more than 10‐fold after ∼ 20 pulses have been applied to the gel, suggesting that a cooperative change in gel structure has occurred. Because there is no concomitant change birefringence must be due to an increase in the number of agarose fibers and /or fiber bundles orienting in the lectric field, which in turn indicates a cooperatice breakdown of the noncovalent “junction zones” that corss‐link the fibers in to the fgel matrix. The sign of the birefringence of LE agarose gels is always positive after extensive junction zone breakdown, indicating that the agarose fibers and fiber bundles preferentially orient parallel to the lectric field when they are freed from the constraints of the gel matrix.
Three other gel‐forming polymers, high electroendosmosis (HEEO) agarose (a more highly changed agarose), β‐carrageenan (a stereoisomer of agarose), and polyacrylamide (a chemically corss‐linked polymer) were alos studied in unidirectional and rapidly reversing electric fields. The birefringence of HEEO agarose backbone chain. The β‐carrageenan gels exhibit variable orientation behavior in reversing electric fields, suggesting that its internal gel structure is not as tightly interconnected as that of agaroise gels. Both HEEO agarose and β‐carrageenan gels exhibit a large increase in the amplitude of the birefringence with increasing pulse number when asymmetric reversing pulses > 7 V/cm are applied to the gels, suggesting that junction zone breakdown in a common feature of polysaccharide gels.
Chemically cross‐linked polyacrylamide gels exhibit very small birefringence signals, indicating that very little orientation occurs in pulsed lectric fields. The sign of the birefringence is independent of the polarity of the lectric field, as expected from the Kerr law, and normal orientation behavior is observed in reversing electric fields. Hence, the anomalous change in sign of the birefringence observed for agarose gels in reversing electric fields must be due to the metastable junction zones in the agarose gel matrix, which allow gel fiber rearrangements to occur. © 1994 John Wiley & Sons, Inc.</description><subject>Analytical biochemistry: general aspects, technics, instrumentation</subject><subject>Analytical, structural and metabolic biochemistry</subject><subject>Biological and medical sciences</subject><subject>Birefringence</subject><subject>Carbohydrate Sequence</subject><subject>Chemical Phenomena</subject><subject>Chemistry, Physical</subject><subject>Electromagnetic Fields</subject><subject>Electrophoresis, Agar Gel - methods</subject><subject>Fundamental and applied biological sciences. Psychology</subject><subject>Gels - chemistry</subject><subject>Molecular Sequence Data</subject><subject>Polymers - chemistry</subject><subject>Sepharose - chemistry</subject><issn>0006-3525</issn><issn>1097-0282</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1994</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp9kM1vEzEQxS0EKqFw5IjkA-K2qb-y9h5pBWmklqKq0KPl9Y5Tg_ej9qZt_vs6yipwquYwh_nNm3kPoY-UzCkh7KT2w5yXhAtSUfEKzSipZEGYYq_RjBBSFnzBFm_Ru5T-ECIEp-QIHclKKMnVDD3cRNMlD92IIYAdo7e49hFc9N0aOgu4d9isTewT4DWENMer1RxfwwPElJF_W85DaBI2XYNt3w4m-tR3-NGPd7gf7yDioQ_bNvedynv0xpmQ4MPUj9Gv799uzs6Li6vl6uzrRWE5VaLgpXCccVXVsnaWKe6Y3BWhNXOkYo2pFHGSsgYawxYi-yWU1rSpleW2cfwYfdnrDrG_30AadeuThRBMB_0maVlKJStZZrDYgzY7Tdm_HqJvTdxqSvQuZ51z1oecM_9pEt7ULTQHego2zz9Pc5OsCS6nbH06YIJRuZeRe-zRB9i-fFOfrn7-_8D0sE8jPB02TfyrS8nlQt_-WGp--_v69Hwp9CV_Bl9kpao</recordid><startdate>199409</startdate><enddate>199409</enddate><creator>Stellwagen, John</creator><creator>Stellwagen, Nancy C.</creator><general>Wiley Subscription Services, Inc., A Wiley Company</general><general>Wiley</general><scope>BSCLL</scope><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>199409</creationdate><title>Transient electric birefringence of agarose gels. II. Reversing electric fields and comparison with other polymer gels</title><author>Stellwagen, John ; Stellwagen, Nancy C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3184-364f32389b7bfc283f27272701b2f092da980f712deda254000011b1db8c3cdf3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1994</creationdate><topic>Analytical biochemistry: general aspects, technics, instrumentation</topic><topic>Analytical, structural and metabolic biochemistry</topic><topic>Biological and medical sciences</topic><topic>Birefringence</topic><topic>Carbohydrate Sequence</topic><topic>Chemical Phenomena</topic><topic>Chemistry, Physical</topic><topic>Electromagnetic Fields</topic><topic>Electrophoresis, Agar Gel - methods</topic><topic>Fundamental and applied biological sciences. Psychology</topic><topic>Gels - chemistry</topic><topic>Molecular Sequence Data</topic><topic>Polymers - chemistry</topic><topic>Sepharose - chemistry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Stellwagen, John</creatorcontrib><creatorcontrib>Stellwagen, Nancy C.</creatorcontrib><collection>Istex</collection><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>Biopolymers</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Stellwagen, John</au><au>Stellwagen, Nancy C.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Transient electric birefringence of agarose gels. II. Reversing electric fields and comparison with other polymer gels</atitle><jtitle>Biopolymers</jtitle><addtitle>Biopolymers</addtitle><date>1994-09</date><risdate>1994</risdate><volume>34</volume><issue>9</issue><spage>1259</spage><epage>1273</epage><pages>1259-1273</pages><issn>0006-3525</issn><eissn>1097-0282</eissn><coden>BIPMAA</coden><abstract>The transient electric birefringence of low electroendosmosis (LE) agarose gels oriented by pulsed unidirectional electric fields was described in detail in Part I [J. Stellwagen and N. C. Stellwagen (1994), Biopolymers, Vol. 34, p. 187]. Here, the birefringence of LE agarose gels in rapidly reversing electric fields, similar in amplitude and duration to those used for field inversion gel electrophoresis, is reported.
Symmetric reversing electric fields cause the sign of the birefringence of LE agarose gels, and hence the direction of orientation of the agarose fibers, to Oscillate in phase with the applied electric field. Because of long‐lasting memory effects, the alternating sign of the birefringence appears to be due to metastable changes in gel structure induced by the electric field. If the reversing field pulses are equal in amplitude but different in duration, the orientation behavior depends critically on the applied voltage. If E < 7 V/cm, the amplitude of the birefringence gradually decreases with increasing pulse number and becomes unmeasurably small. However, if E > 7 V/cm, the amplitude of the birefringence increase more than 10‐fold after ∼ 20 pulses have been applied to the gel, suggesting that a cooperative change in gel structure has occurred. Because there is no concomitant change birefringence must be due to an increase in the number of agarose fibers and /or fiber bundles orienting in the lectric field, which in turn indicates a cooperatice breakdown of the noncovalent “junction zones” that corss‐link the fibers in to the fgel matrix. The sign of the birefringence of LE agarose gels is always positive after extensive junction zone breakdown, indicating that the agarose fibers and fiber bundles preferentially orient parallel to the lectric field when they are freed from the constraints of the gel matrix.
Three other gel‐forming polymers, high electroendosmosis (HEEO) agarose (a more highly changed agarose), β‐carrageenan (a stereoisomer of agarose), and polyacrylamide (a chemically corss‐linked polymer) were alos studied in unidirectional and rapidly reversing electric fields. The birefringence of HEEO agarose backbone chain. The β‐carrageenan gels exhibit variable orientation behavior in reversing electric fields, suggesting that its internal gel structure is not as tightly interconnected as that of agaroise gels. Both HEEO agarose and β‐carrageenan gels exhibit a large increase in the amplitude of the birefringence with increasing pulse number when asymmetric reversing pulses > 7 V/cm are applied to the gels, suggesting that junction zone breakdown in a common feature of polysaccharide gels.
Chemically cross‐linked polyacrylamide gels exhibit very small birefringence signals, indicating that very little orientation occurs in pulsed lectric fields. The sign of the birefringence is independent of the polarity of the lectric field, as expected from the Kerr law, and normal orientation behavior is observed in reversing electric fields. Hence, the anomalous change in sign of the birefringence observed for agarose gels in reversing electric fields must be due to the metastable junction zones in the agarose gel matrix, which allow gel fiber rearrangements to occur. © 1994 John Wiley & Sons, Inc.</abstract><cop>Hoboken</cop><pub>Wiley Subscription Services, Inc., A Wiley Company</pub><pmid>7948738</pmid><doi>10.1002/bip.360340914</doi><tpages>15</tpages></addata></record> |
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subjects | Analytical biochemistry: general aspects, technics, instrumentation Analytical, structural and metabolic biochemistry Biological and medical sciences Birefringence Carbohydrate Sequence Chemical Phenomena Chemistry, Physical Electromagnetic Fields Electrophoresis, Agar Gel - methods Fundamental and applied biological sciences. Psychology Gels - chemistry Molecular Sequence Data Polymers - chemistry Sepharose - chemistry |
title | Transient electric birefringence of agarose gels. II. Reversing electric fields and comparison with other polymer gels |
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