In this work hydrogen bonding in a diverse set of 36 unnatural and the three natural Watson Crick base pairs adenine (A)–thymine (T), adenine (A)–uracil (U) and guanine (G)–cytosine (C) was assessed utilizing local vibrational force constants derived from the local mode analysis, originally introduced by Konkoli and Cremer as a unique bond strength measure based on vibrational spectroscopy. The local mode analysis was complemented by the topological analysis of the electronic density and the natural bond orbital analysis. The most interesting findings of our study are that (i) hydrogen bonding in Watson Crick base pairs is not exceptionally strong and (ii) the N–H⋯N is the most favorable hydrogen bond in both unnatural and natural base pairs while O–H⋯N/O bonds are the less favorable in unnatural base pairs and not found at all in natural base pairs. In addition, the important role of non-classical C–H⋯N/O bonds for the stabilization of base pairs was revealed, especially the role of C–H⋯O bonds in Watson Crick base pairs. Hydrogen bonding in Watson Crick base pairs modeled in the DNA via a QM/MM approach showed that the DNA environment increases the strength of the central N–H⋯N bond and the C–H⋯O bonds, and at the same time decreases the strength of the N–H⋯O bond. However, the general trends observed in the gas phase calculations remain unchanged. The new methodology presented and tested in this work provides the bioengineering community with an efficient design tool to assess and predict the type and strength of hydrogen bonding in artificial base pairs.
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Anionic G•U pairs in bacterial ribosomal rRNAs
Wobble GU pairs (or G•U) occur frequently within double-stranded RNA helices interspersed between standard G=C and A-U Watson-Crick pairs. Another type of G•U pair interacting via their Watson-Crick edges has been observed in the A site of ribosome structures between a modified U34 in the tRNA anticodon triplet and G+3 in the mRNA. In such pairs the electronic structure of the U is changed with a negative charge on N3(U), resulting in two H-bonds between N1(G)…O4(U) and N2(G)…N3(U). Here, we report that such pairs occur in other highly conserved positions in ribosomal RNAs of bacteria in the absence of U modification. An anionic cis Watson-Crick G•G pair is also observed and well conserved in the small subunit. These pairs are observed in tightly folded regions.
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- Award ID(s):
- 2002182
- PAR ID:
- 10416900
- Date Published:
- Journal Name:
- RNA
- ISSN:
- 1355-8382
- Page Range / eLocation ID:
- rna.079583.123
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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Abstract 8‐Oxoguanosine is the most common oxidatively generated base damage and pairs with complementary cytidine within duplex DNA. The 8‐oxoguanosine−cytidine lesion, if not recognized and removed, not only leads to G‐to‐T transversion mutations but renders the base pair being more vulnerable to the ionizing radiation and singlet oxygen (1O2) damage. Herein, reaction dynamics of a prototype Watson−Crick base pair [9MOG ⋅ 1MC]⋅+, consisting of 9‐methyl‐8‐oxoguanine radical cation (9MOG⋅+) and 1‐methylcystosine (1MC), was examined using mass spectrometry coupled with electrospray ionization. We first detected base‐pair dissociation in collisions with the Xe gas, which provided insight into intra‐base pair proton transfer of 9MOG⋅+ ⋅ 1MC[9MOG − HN1]⋅ ⋅ [1MC+HN3′]+and subsequent non‐statistical base‐pair separation. We then measured the reaction of [9MOG ⋅ 1MC]⋅+with1O2, revealing the two most probable pathways, C5‐O2addition and HN7‐abstraction at 9MOG. Reactions were entangled with the two forms of 9MOG radicals and base‐pair structures as well as multi‐configurations between open‐shell radicals and1O2(that has a mixed singlet/triplet character). These were disentangled by utilizing approximately spin‐projected density functional theory, coupled‐cluster theory and multi‐referential electronic structure modeling. The work delineated base‐pair structural context effects and determined relative reactivity toward1O2as [9MOG − H]⋅>9MOG⋅+>[9MOG − HN1]⋅ ⋅ [1MC+HN3′]+≥9MOG⋅+ ⋅ 1MC.more » « less
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