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Improved Parameters for the Prediction of RNA Hairpin Stability
Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type where XY is the set of four Watson−Crick base pairs and the underlined loop sequences are three to nine nucleotides. A nearest neighbor analysis of the data indicates the free energy of loop formatio...
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Published in: | Biochemistry (Easton) 1997-04, Vol.36 (16), p.4844-4851 |
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description | Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type where XY is the set of four Watson−Crick base pairs and the underlined loop sequences are three to nine nucleotides. A nearest neighbor analysis of the data indicates the free energy of loop formation at 37 °C is dependent upon loop size and closing base pair. The model previously developed to predict the stability for RNA hairpin loops (n > 3) includes contributions from the size of the loop, the identity of the closing base pair, the free energy increment (ΔG°37mm) for the interaction of the closing base pair with the first mismatch and an additional stabilization term for GA and UU first mismatches [Serra, M. J., Axenson, T. J., & Turner, D. H. (1994) Biochemistry 33, 14289]. The results presented here allow improvements in the parameters used to predict RNA hairpin stability. For hairpin loops of n = 4−9, ΔG°37iL(n) is 4.9, 5.0, 5.0, 5.0, 4.9, and 5.5 kcal/mol, respectively, and the penalty for hairpin closure by AU or UA is +0.6 kcal/mol. ΔG°37iL(n) is the free energy for initiating a loop of n nucleotides. The model for predicting hairpin loop stability for loops larger than three becomes ΔG°37L(n) = ΔG°37iL(n) + ΔG°37mm + 0.6(if closed by AU or UA) −0.7(if first mismatch is GA or UU). Hairpin loops of three are modeled as independent of loop sequence with ΔG°37iL(3) = 4.8 and the penalty for AU closure of +0.6 kcal/mol. Thermodynamic parameters for hairpin formation in 1 M NaCl for 11 naturally occurring RNA hairpin sequences are reported. The model provides good agreement with the measured values for both T M (within 10 °C of the measured value) and ΔG°37 (within 0.8 kcal/mol of the measured value) for hairpin formation. In general, the nearest neighbor model allows prediction of RNA hairpin stability to within 5−10% of the experimentally measured values. |
doi_str_mv | 10.1021/bi962608j |
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A nearest neighbor analysis of the data indicates the free energy of loop formation at 37 °C is dependent upon loop size and closing base pair. The model previously developed to predict the stability for RNA hairpin loops (n > 3) includes contributions from the size of the loop, the identity of the closing base pair, the free energy increment (ΔG°37mm) for the interaction of the closing base pair with the first mismatch and an additional stabilization term for GA and UU first mismatches [Serra, M. J., Axenson, T. J., & Turner, D. H. (1994) Biochemistry 33, 14289]. The results presented here allow improvements in the parameters used to predict RNA hairpin stability. For hairpin loops of n = 4−9, ΔG°37iL(n) is 4.9, 5.0, 5.0, 5.0, 4.9, and 5.5 kcal/mol, respectively, and the penalty for hairpin closure by AU or UA is +0.6 kcal/mol. ΔG°37iL(n) is the free energy for initiating a loop of n nucleotides. The model for predicting hairpin loop stability for loops larger than three becomes ΔG°37L(n) = ΔG°37iL(n) + ΔG°37mm + 0.6(if closed by AU or UA) −0.7(if first mismatch is GA or UU). Hairpin loops of three are modeled as independent of loop sequence with ΔG°37iL(3) = 4.8 and the penalty for AU closure of +0.6 kcal/mol. Thermodynamic parameters for hairpin formation in 1 M NaCl for 11 naturally occurring RNA hairpin sequences are reported. The model provides good agreement with the measured values for both T M (within 10 °C of the measured value) and ΔG°37 (within 0.8 kcal/mol of the measured value) for hairpin formation. In general, the nearest neighbor model allows prediction of RNA hairpin stability to within 5−10% of the experimentally measured values.</description><identifier>ISSN: 0006-2960</identifier><identifier>EISSN: 1520-4995</identifier><identifier>DOI: 10.1021/bi962608j</identifier><identifier>PMID: 9125504</identifier><language>eng</language><publisher>United States: American Chemical Society</publisher><subject>Models, Chemical ; Nucleic Acid Conformation ; RNA - chemistry ; Thermodynamics</subject><ispartof>Biochemistry (Easton), 1997-04, Vol.36 (16), p.4844-4851</ispartof><rights>Copyright © 1997 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a445t-8c3857945f1b8fc42cbed7586901bf39599503a6efd428fa02653790bc9bf07c3</citedby><cites>FETCH-LOGICAL-a445t-8c3857945f1b8fc42cbed7586901bf39599503a6efd428fa02653790bc9bf07c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/9125504$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Serra, Martin J</creatorcontrib><creatorcontrib>Barnes, Thomas W</creatorcontrib><creatorcontrib>Betschart, Kelly</creatorcontrib><creatorcontrib>Gutierrez, Mathew J</creatorcontrib><creatorcontrib>Sprouse, Kimberly J</creatorcontrib><creatorcontrib>Riley, Cheryl K</creatorcontrib><creatorcontrib>Stewart, Lora</creatorcontrib><creatorcontrib>Temel, Ryan E</creatorcontrib><title>Improved Parameters for the Prediction of RNA Hairpin Stability</title><title>Biochemistry (Easton)</title><addtitle>Biochemistry</addtitle><description>Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type where XY is the set of four Watson−Crick base pairs and the underlined loop sequences are three to nine nucleotides. A nearest neighbor analysis of the data indicates the free energy of loop formation at 37 °C is dependent upon loop size and closing base pair. The model previously developed to predict the stability for RNA hairpin loops (n > 3) includes contributions from the size of the loop, the identity of the closing base pair, the free energy increment (ΔG°37mm) for the interaction of the closing base pair with the first mismatch and an additional stabilization term for GA and UU first mismatches [Serra, M. J., Axenson, T. J., & Turner, D. H. (1994) Biochemistry 33, 14289]. The results presented here allow improvements in the parameters used to predict RNA hairpin stability. For hairpin loops of n = 4−9, ΔG°37iL(n) is 4.9, 5.0, 5.0, 5.0, 4.9, and 5.5 kcal/mol, respectively, and the penalty for hairpin closure by AU or UA is +0.6 kcal/mol. ΔG°37iL(n) is the free energy for initiating a loop of n nucleotides. The model for predicting hairpin loop stability for loops larger than three becomes ΔG°37L(n) = ΔG°37iL(n) + ΔG°37mm + 0.6(if closed by AU or UA) −0.7(if first mismatch is GA or UU). Hairpin loops of three are modeled as independent of loop sequence with ΔG°37iL(3) = 4.8 and the penalty for AU closure of +0.6 kcal/mol. Thermodynamic parameters for hairpin formation in 1 M NaCl for 11 naturally occurring RNA hairpin sequences are reported. The model provides good agreement with the measured values for both T M (within 10 °C of the measured value) and ΔG°37 (within 0.8 kcal/mol of the measured value) for hairpin formation. In general, the nearest neighbor model allows prediction of RNA hairpin stability to within 5−10% of the experimentally measured values.</description><subject>Models, Chemical</subject><subject>Nucleic Acid Conformation</subject><subject>RNA - chemistry</subject><subject>Thermodynamics</subject><issn>0006-2960</issn><issn>1520-4995</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1997</creationdate><recordtype>article</recordtype><recordid>eNqFkE1LAzEQhoMotVYP_gBhLwoeVifZfGxOUvxqQbRoPYdsNsHUbrcmW9F_b6SlJ8HTMLwPMy8PQscYLjAQfFl5yQmHcraD-pgRyKmUbBf1AYDnRHLYRwcxztJKQdAe6klMGAPaR1fjZhnaT1tnEx10YzsbYubakHVvNpsEW3vT-XaRtS57fhxmI-3D0i-yl05Xfu6770O05_Q82qPNHKDXu9vp9Sh_eLofXw8fck0p6_LSFCUTkjKHq9IZSkxla8FKLgFXrpAs9YVCc-tqSkqngXBWCAmVkZUDYYoBOlvfTW0_VjZ2qvHR2PlcL2y7ikqUUhaCkX9BzEFICTyB52vQhDbGYJ1aBt_o8K0wqF-rams1sSebo6uqsfWW3GhMeb7Ofezs1zbW4V1xkWqp6eRF3TwXd6Obx0LJxJ-ueW2imrWrsEju_vj7A3mEi1Q</recordid><startdate>19970422</startdate><enddate>19970422</enddate><creator>Serra, Martin J</creator><creator>Barnes, Thomas W</creator><creator>Betschart, Kelly</creator><creator>Gutierrez, Mathew J</creator><creator>Sprouse, Kimberly J</creator><creator>Riley, Cheryl K</creator><creator>Stewart, Lora</creator><creator>Temel, Ryan E</creator><general>American Chemical Society</general><scope>BSCLL</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>7TM</scope><scope>7X8</scope></search><sort><creationdate>19970422</creationdate><title>Improved Parameters for the Prediction of RNA Hairpin Stability</title><author>Serra, Martin J ; Barnes, Thomas W ; Betschart, Kelly ; Gutierrez, Mathew J ; Sprouse, Kimberly J ; Riley, Cheryl K ; Stewart, Lora ; Temel, Ryan E</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a445t-8c3857945f1b8fc42cbed7586901bf39599503a6efd428fa02653790bc9bf07c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1997</creationdate><topic>Models, Chemical</topic><topic>Nucleic Acid Conformation</topic><topic>RNA - chemistry</topic><topic>Thermodynamics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Serra, Martin J</creatorcontrib><creatorcontrib>Barnes, Thomas W</creatorcontrib><creatorcontrib>Betschart, Kelly</creatorcontrib><creatorcontrib>Gutierrez, Mathew J</creatorcontrib><creatorcontrib>Sprouse, Kimberly J</creatorcontrib><creatorcontrib>Riley, Cheryl K</creatorcontrib><creatorcontrib>Stewart, Lora</creatorcontrib><creatorcontrib>Temel, Ryan E</creatorcontrib><collection>Istex</collection><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>Nucleic Acids Abstracts</collection><collection>MEDLINE - Academic</collection><jtitle>Biochemistry (Easton)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Serra, Martin J</au><au>Barnes, Thomas W</au><au>Betschart, Kelly</au><au>Gutierrez, Mathew J</au><au>Sprouse, Kimberly J</au><au>Riley, Cheryl K</au><au>Stewart, Lora</au><au>Temel, Ryan E</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Improved Parameters for the Prediction of RNA Hairpin Stability</atitle><jtitle>Biochemistry (Easton)</jtitle><addtitle>Biochemistry</addtitle><date>1997-04-22</date><risdate>1997</risdate><volume>36</volume><issue>16</issue><spage>4844</spage><epage>4851</epage><pages>4844-4851</pages><issn>0006-2960</issn><eissn>1520-4995</eissn><abstract>Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type where XY is the set of four Watson−Crick base pairs and the underlined loop sequences are three to nine nucleotides. A nearest neighbor analysis of the data indicates the free energy of loop formation at 37 °C is dependent upon loop size and closing base pair. The model previously developed to predict the stability for RNA hairpin loops (n > 3) includes contributions from the size of the loop, the identity of the closing base pair, the free energy increment (ΔG°37mm) for the interaction of the closing base pair with the first mismatch and an additional stabilization term for GA and UU first mismatches [Serra, M. J., Axenson, T. J., & Turner, D. H. (1994) Biochemistry 33, 14289]. The results presented here allow improvements in the parameters used to predict RNA hairpin stability. For hairpin loops of n = 4−9, ΔG°37iL(n) is 4.9, 5.0, 5.0, 5.0, 4.9, and 5.5 kcal/mol, respectively, and the penalty for hairpin closure by AU or UA is +0.6 kcal/mol. ΔG°37iL(n) is the free energy for initiating a loop of n nucleotides. The model for predicting hairpin loop stability for loops larger than three becomes ΔG°37L(n) = ΔG°37iL(n) + ΔG°37mm + 0.6(if closed by AU or UA) −0.7(if first mismatch is GA or UU). Hairpin loops of three are modeled as independent of loop sequence with ΔG°37iL(3) = 4.8 and the penalty for AU closure of +0.6 kcal/mol. Thermodynamic parameters for hairpin formation in 1 M NaCl for 11 naturally occurring RNA hairpin sequences are reported. The model provides good agreement with the measured values for both T M (within 10 °C of the measured value) and ΔG°37 (within 0.8 kcal/mol of the measured value) for hairpin formation. In general, the nearest neighbor model allows prediction of RNA hairpin stability to within 5−10% of the experimentally measured values.</abstract><cop>United States</cop><pub>American Chemical Society</pub><pmid>9125504</pmid><doi>10.1021/bi962608j</doi><tpages>8</tpages></addata></record> |
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subjects | Models, Chemical Nucleic Acid Conformation RNA - chemistry Thermodynamics |
title | Improved Parameters for the Prediction of RNA Hairpin Stability |
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