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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
Main Authors: Serra, Martin J, Barnes, Thomas W, Betschart, Kelly, Gutierrez, Mathew J, Sprouse, Kimberly J, Riley, Cheryl K, Stewart, Lora, Temel, Ryan E
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container_end_page 4851
container_issue 16
container_start_page 4844
container_title Biochemistry (Easton)
container_volume 36
creator Serra, Martin J
Barnes, Thomas W
Betschart, Kelly
Gutierrez, Mathew J
Sprouse, Kimberly J
Riley, Cheryl K
Stewart, Lora
Temel, Ryan E
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.
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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 &gt; 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., &amp; 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. 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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 &gt; 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., &amp; 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. 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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 &gt; 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., &amp; 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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source American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list)
subjects Models, Chemical
Nucleic Acid Conformation
RNA - chemistry
Thermodynamics
title Improved Parameters for the Prediction of RNA Hairpin Stability
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