Protein–Surfactant Interaction: Sodium Dodecyl Sulfate-Induced Unfolding of Ribonuclease A
Protein–surfactant interaction is widely studied to understand stability and structural changes in proteins. In this Article, we have investigated SDS-induced unfolding of RNase A using absorbance, intrinsic fluorescence of the protein, anisotropy, TNS fluorescence, and near- and far-UV circular dic...
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Veröffentlicht in: | The journal of physical chemistry. B 2011-12, Vol.115 (49), p.14760-14767 |
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description | Protein–surfactant interaction is widely studied to understand stability and structural changes in proteins. In this Article, we have investigated SDS-induced unfolding of RNase A using absorbance, intrinsic fluorescence of the protein, anisotropy, TNS fluorescence, and near- and far-UV circular dichroism. Unfolding titration curves obtained from the absorbance and fluorescence changes were fitted into a five-state protein unfolding model by assuming formation of three intermediate states. Free energy changes and m-values of all four transitions between the native and unfolded state were evaluated. The transitions are categorized into two different regions. Region I, up to 0.5 mM of SDS, involves ionic interaction between the protein and SDS where the secondary and tertiary structure of the protein is altered to a less extent. In region II, hydrophobic interaction dominates and has two distinct transitions. The first transition arises from the aggregation of surfactant molecules around the protein hydrophobic sites. In the following transition, the micelles probably expand more, and a few more hydrophobic sites are occupied by the surfactant. In this region, the tertiary contacts are completely broken, and almost 50% of the secondary structure is lost. The aggregation of SDS around the protein starts well below the CMC. These conformational changes can be explained by the necklace and beads model, and the free energy of formation of such a complex for the RNase A–SDS system is found to be 5.2 (±1.0) kcal mol–1. The probable interaction sites and the mechanism of unfolding have been discussed in detail. |
doi_str_mv | 10.1021/jp2062496 |
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In this Article, we have investigated SDS-induced unfolding of RNase A using absorbance, intrinsic fluorescence of the protein, anisotropy, TNS fluorescence, and near- and far-UV circular dichroism. Unfolding titration curves obtained from the absorbance and fluorescence changes were fitted into a five-state protein unfolding model by assuming formation of three intermediate states. Free energy changes and m-values of all four transitions between the native and unfolded state were evaluated. The transitions are categorized into two different regions. Region I, up to 0.5 mM of SDS, involves ionic interaction between the protein and SDS where the secondary and tertiary structure of the protein is altered to a less extent. In region II, hydrophobic interaction dominates and has two distinct transitions. The first transition arises from the aggregation of surfactant molecules around the protein hydrophobic sites. In the following transition, the micelles probably expand more, and a few more hydrophobic sites are occupied by the surfactant. In this region, the tertiary contacts are completely broken, and almost 50% of the secondary structure is lost. The aggregation of SDS around the protein starts well below the CMC. These conformational changes can be explained by the necklace and beads model, and the free energy of formation of such a complex for the RNase A–SDS system is found to be 5.2 (±1.0) kcal mol–1. 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B</title><addtitle>J. Phys. Chem. B</addtitle><description>Protein–surfactant interaction is widely studied to understand stability and structural changes in proteins. In this Article, we have investigated SDS-induced unfolding of RNase A using absorbance, intrinsic fluorescence of the protein, anisotropy, TNS fluorescence, and near- and far-UV circular dichroism. Unfolding titration curves obtained from the absorbance and fluorescence changes were fitted into a five-state protein unfolding model by assuming formation of three intermediate states. Free energy changes and m-values of all four transitions between the native and unfolded state were evaluated. The transitions are categorized into two different regions. Region I, up to 0.5 mM of SDS, involves ionic interaction between the protein and SDS where the secondary and tertiary structure of the protein is altered to a less extent. In region II, hydrophobic interaction dominates and has two distinct transitions. The first transition arises from the aggregation of surfactant molecules around the protein hydrophobic sites. In the following transition, the micelles probably expand more, and a few more hydrophobic sites are occupied by the surfactant. In this region, the tertiary contacts are completely broken, and almost 50% of the secondary structure is lost. The aggregation of SDS around the protein starts well below the CMC. These conformational changes can be explained by the necklace and beads model, and the free energy of formation of such a complex for the RNase A–SDS system is found to be 5.2 (±1.0) kcal mol–1. The probable interaction sites and the mechanism of unfolding have been discussed in detail.</description><subject>Absorbance</subject><subject>Agglomeration</subject><subject>Animals</subject><subject>Anisotropy</subject><subject>B: Biophysical Chemistry</subject><subject>Beads</subject><subject>Cattle</subject><subject>Circular Dichroism</subject><subject>Fluorescence</subject><subject>Hydrophobic and Hydrophilic Interactions</subject><subject>Protein Structure, Secondary</subject><subject>Protein Unfolding</subject><subject>Proteins</subject><subject>Ribonuclease, Pancreatic - chemistry</subject><subject>Sodium</subject><subject>Sodium Dodecyl Sulfate - chemistry</subject><subject>Spectrometry, Fluorescence</subject><subject>Surface-Active Agents - chemistry</subject><subject>Surfactants</subject><issn>1520-6106</issn><issn>1520-5207</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNp90L1KBDEQB_Agit-FLyDbiFqsJrkke2t3-HkgKJ52wpKdTGSPveRMNoWd7-Ab-iSu3GklFsMMzI9_8Sdkj9ETRjk7nc45VVyUaoVsMslp3k-xurwVo2qDbMU4pZRLPlTrZINzygRTdJM83wffYeM-3z8mKVgNnXZdNnYdhv5uvDvLJt40aZZdeIPw1maT1FrdYT52JgGa7MlZ35rGvWTeZg9N7V2CFnXEbLRD1qxuI-4u9zZ5urp8PL_Jb--ux-ej21wLNujyWg4NgEZRl1ijLWEAoJg1SiMFS60oJSsKAMHrQkklhQFZFgXSeth_wAy2yeEidx78a8LYVbMmAratduhTrErGSsHpUPTy6F_JCjmQTBTsmx4vKAQfY0BbzUMz0-GtYrT6rr36rb23-8vYVM_Q_MqfnntwsAAaYjX1Kbi-jz-CvgBOkYox</recordid><startdate>20111215</startdate><enddate>20111215</enddate><creator>Tejaswi Naidu, K</creator><creator>Prakash Prabhu, N</creator><general>American Chemical Society</general><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>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope><scope>7X8</scope></search><sort><creationdate>20111215</creationdate><title>Protein–Surfactant Interaction: Sodium Dodecyl Sulfate-Induced Unfolding of Ribonuclease A</title><author>Tejaswi Naidu, K ; Prakash Prabhu, N</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a413t-b58dccae4b9ebef9c3cc61fd6ae0cf0f495177cc42b765654dc5977e0b8951cd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Absorbance</topic><topic>Agglomeration</topic><topic>Animals</topic><topic>Anisotropy</topic><topic>B: Biophysical Chemistry</topic><topic>Beads</topic><topic>Cattle</topic><topic>Circular Dichroism</topic><topic>Fluorescence</topic><topic>Hydrophobic and Hydrophilic Interactions</topic><topic>Protein Structure, Secondary</topic><topic>Protein Unfolding</topic><topic>Proteins</topic><topic>Ribonuclease, Pancreatic - chemistry</topic><topic>Sodium</topic><topic>Sodium Dodecyl Sulfate - chemistry</topic><topic>Spectrometry, Fluorescence</topic><topic>Surface-Active Agents - chemistry</topic><topic>Surfactants</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tejaswi Naidu, K</creatorcontrib><creatorcontrib>Prakash Prabhu, N</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><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><jtitle>The journal of physical chemistry. B</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tejaswi Naidu, K</au><au>Prakash Prabhu, N</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Protein–Surfactant Interaction: Sodium Dodecyl Sulfate-Induced Unfolding of Ribonuclease A</atitle><jtitle>The journal of physical chemistry. B</jtitle><addtitle>J. Phys. Chem. B</addtitle><date>2011-12-15</date><risdate>2011</risdate><volume>115</volume><issue>49</issue><spage>14760</spage><epage>14767</epage><pages>14760-14767</pages><issn>1520-6106</issn><eissn>1520-5207</eissn><abstract>Protein–surfactant interaction is widely studied to understand stability and structural changes in proteins. In this Article, we have investigated SDS-induced unfolding of RNase A using absorbance, intrinsic fluorescence of the protein, anisotropy, TNS fluorescence, and near- and far-UV circular dichroism. Unfolding titration curves obtained from the absorbance and fluorescence changes were fitted into a five-state protein unfolding model by assuming formation of three intermediate states. Free energy changes and m-values of all four transitions between the native and unfolded state were evaluated. The transitions are categorized into two different regions. Region I, up to 0.5 mM of SDS, involves ionic interaction between the protein and SDS where the secondary and tertiary structure of the protein is altered to a less extent. In region II, hydrophobic interaction dominates and has two distinct transitions. The first transition arises from the aggregation of surfactant molecules around the protein hydrophobic sites. In the following transition, the micelles probably expand more, and a few more hydrophobic sites are occupied by the surfactant. In this region, the tertiary contacts are completely broken, and almost 50% of the secondary structure is lost. The aggregation of SDS around the protein starts well below the CMC. These conformational changes can be explained by the necklace and beads model, and the free energy of formation of such a complex for the RNase A–SDS system is found to be 5.2 (±1.0) kcal mol–1. The probable interaction sites and the mechanism of unfolding have been discussed in detail.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>22014160</pmid><doi>10.1021/jp2062496</doi><tpages>8</tpages></addata></record> |
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subjects | Absorbance Agglomeration Animals Anisotropy B: Biophysical Chemistry Beads Cattle Circular Dichroism Fluorescence Hydrophobic and Hydrophilic Interactions Protein Structure, Secondary Protein Unfolding Proteins Ribonuclease, Pancreatic - chemistry Sodium Sodium Dodecyl Sulfate - chemistry Spectrometry, Fluorescence Surface-Active Agents - chemistry Surfactants |
title | Protein–Surfactant Interaction: Sodium Dodecyl Sulfate-Induced Unfolding of Ribonuclease A |
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