Vokácová Zuzana, Bickelhaupt F Matthias, Sponer JiYí, Sychrovský Vladimír
Institute of Organic Chemistry and Biochemistry, v.v.i., Academy of Sciences of the Czech Republic, Flemingovo Square 2, 166 10 Prague 6, Czech Republic.
J Phys Chem A. 2009 Jul 23;113(29):8379-86. doi: 10.1021/jp902473v.
The (3)J(C8-H1'), (3)J(C4-H1'), (1)J(C8-H8), (1)J(C1'-H1'), (1)J(C2'-H2'), and (1)J(C2'-H2'2) indirect scalar coupling constants were calculated with the density functional theory in the deoxyguanosine and riboguanosine molecules. The following geometry descriptors were considered in analysis of the structural dependence of the six J couplings: the glycosidic torsion angle chi and conformation of the hydroxymethyl group at the C4' carbon of sugar mimicking the backbone residue and the sugar pucker (C2'-, C3'-endo). The (3)J(C8-H1') and (3)J(C4-H1') couplings, which are typically assigned to the chi torsion, also depended on the sugar pucker, although the calculated dependence of the latter coupling on sugar pucker was nearly negligible. New parametrization of the Karplus equations, taking into account the stereoinversion effect at the glycosidic nitrogen atom and solvent effects, was calculated for the (3)J(C8-H1') and (3)J(C4-H1') coupling assigned to the chi torsion. The calculated phase shift of chi torsion angle in these new Karplus equations was larger by approximately 10 degrees compared to its commonly accepted value of 60 degrees (Wijmenga, S. S.; van Buuren, B. N. M. Prog. NMR Spectrosc. 1998, 32, 287.). The calculated (1)J(C2'-H2') and (1)J(C2'-H2'2) coupling dominantly depended on the sugar type (deoxyribose or ribose) and its pucker, while the (1)J(C1'-H1') and (1)J(C8-H8) coupling dominantly depended on the glycosidic torsion angle, although quantitatively, all four (1)J couplings depended on both geometry parameters. The dependences of j-couplings on the torsion angle chi calculated in isolated nucleosides were compared with those taking into account the effect of base pairing occurring in the WC/SE RNA base pair family, which appeared to be minor. The calculated (3)J couplings agreed well with available experimental data similarly as the (1)J couplings, although lack of experimental data diminished more reliable validation of the later couplings.
利用密度泛函理论计算了脱氧鸟苷和核糖鸟苷分子中的(3)J(C8-H1')、(3)J(C4-H1')、(1)J(C8-H8)、(1)J(C1'-H1')、(1)J(C2'-H2')和(1)J(C2'-H2'2)间接标量耦合常数。在分析这六种J耦合的结构依赖性时考虑了以下几何描述符:糖苷扭转角χ、模拟主链残基的糖的C4'碳上羟甲基的构象以及糖的折叠(C2'-、C3'-内型)。通常归因于χ扭转的(3)J(C8-H1')和(3)J(C4-H1')耦合也取决于糖的折叠,尽管计算得出的后者耦合对糖折叠的依赖性几乎可以忽略不计。考虑到糖苷氮原子处的立体反转效应和溶剂效应,对归因于χ扭转的(3)J(C8-H1')和(3)J(C4-H1')耦合计算了Karplus方程的新参数化。在这些新的Karplus方程中计算出的χ扭转角的相移比其通常接受的值60度大约大10度(维门加,S.S.;范布伦,B.N.M.《核磁共振光谱进展》1998年,32卷,287页)。计算出的(1)J(C2'-H2')和(1)J(C2'-H2'2)耦合主要取决于糖的类型(脱氧核糖或核糖)及其折叠,而(1)J(C1'-H1')和(1)J(C8-H8)耦合主要取决于糖苷扭转角,尽管从数量上看,所有这四种(1)J耦合都取决于这两个几何参数。将在孤立核苷中计算出的J耦合对扭转角χ的依赖性与考虑了WC/SE RNA碱基对家族中碱基配对效应的依赖性进行了比较,结果显示这种效应较小。计算出的(3)J耦合与现有实验数据吻合良好,(1)J耦合也是如此,尽管缺乏实验数据减少了对后一种耦合更可靠的验证。