Effects of Base Substitutions in an RNA Hairpin from Molecular Dynamics and Free Energy Simulations

• Published in: Biophysical journal 2003-12, Vol.85 (6), p.3445-3459
• Main Authors: Sarzynska, Joanna, Nilsson, Lennart, Kulinski, Tadeusz
• Format: Article
• Language: English
• Subjects: Adenosine - chemistry; Biophysical Theory and Modeling; Carbohydrates - chemistry; Computer Simulation; Hydrogen Bonding; Inosine - chemistry; Ions; Magnetic Resonance Spectroscopy; Medicin och hälsovetenskap; Models, Molecular; Molecular biology; Molecules; Mutation; NMR; Nuclear magnetic resonance; Nucleic Acid Conformation; Protein Structure, Tertiary; Ribonucleic acid; RNA; RNA - chemistry; Sodium - chemistry; Temperature; Thermodynamics; Time Factors; Water - chemistry
• ISSN: 0006-3495; 1542-0086
• DOI: 10.1016/S0006-3495(03)74766-3

Contributions of individual interactions in the GGC GCAAGCC hairpin containing a GCAA tetraloop were studied by computer simulations using base substitutions. The G in the first tetraloop position was replaced by inosine (I) or adenosine (A), and the G in the C-G basepair closing the tetraloop was replaced by I. These substitutions eliminate particular hydrogen bonds proposed in the nuclear magnetic resonance model of the GCAA tetraloop. Molecular dynamics simulations of the GCAA tetraloop in aqueous solvent displayed a well-defined hydrogen pattern between the first and last loop nucleotides (G and A) stabilized by a bridging water molecule. Substitution of G→I in the basepair closing the tetraloop did not significantly influence the loop structure and dynamics. The ICAA loop maintained the overall structure, but displayed variation in the hydrogen-bond network within the tetraloop itself. Molecular dynamics simulations of the ACAA loop led to conformational heterogeneity of the resulting structures. Changes of hairpin formation free energy associated with substitutions of individual bases were calculated by the free energy perturbation method. The calculated decrease of the hairpin stability upon G→I substitution in the C-G basepair closing the tetraloop was in good agreement with experimental thermodynamic data. Our theoretical estimates for G→I and G→A mutations located in the tetraloop suggest larger loop destabilization than corresponding experimental results. The extent of conformational sampling of the structures resulting from base substitutions and its impact on the calculated free energy was discussed.