Olmsted M C, Anderson C F, Record M T
Department of Chemistry, University of Wisconsin-Madison 53706.
Biopolymers. 1991 Nov;31(13):1593-604. doi: 10.1002/bip.360311314.
Effects of salt concentration on the stabilities of oligonucleotide helices are analyzed directly in terms of delta gamma N----yN identical to gamma denyN - gamma natN, the difference in the salt-nucleotide phosphate preferential interaction coefficients for the denatured state, having yN phosphate charges, and for the native state, having N phosphate charges (y = 1 for hairpin denaturation and y = 0.5 for dimer denaturation). Previous experimental studies of the denaturation of hairpin oligonucleotides (having 18 less than N less than 44) indicate significant differences between delta gamma N----N and delta gamma infinity, the value determined for the denaturation of the corresponding polynucleotide. These differences are thermodynamic manifestations of the oligoelectrolyte end effect. In contrast, the available data on the denaturation of oligonucleotide dimer helices (N less than or equal to 22) imply that differences between delta gamma infinity and delta gamma N----0.5N, and hence oligoelectrolyte end effects, are small or negligible. To determine the origin of these apparently conflicting implications concerning the importance of oligoelectrolyte end effects, we have calculated the N dependence of gamma N from grand canonical Monte Carlo simulations for an idealized model of the structure and charge distribution of each oligomer conformation. Our calculations are in quantitative agreement with the experimental finding for d(TA) hairpin oligomers that -delta gamma N----N decreases linearly as N-1 increases, and with the extant experimental determinations of delta gamma N----0.5N. These results provide an illustration of how the large electrostatic end effects exhibited by the hairpin denaturation data are masked when delta gamma infinity is compared with values of delta gamma N----0.5N for short dimer helices (N less than or equal to 22). For 0.5N greater than 24, -delta gamma N----0.5N is predicted to be a linear function of N-1 whose slope has the opposite sign from, and is more salt-concentration dependent than, the corresponding slope of -delta gamma N----N as a function of N-1. Our calculations also yield predictions about the N dependences of the individual values of gamma N that can be tested by determining Donnan coefficients from membrane dialysis equilibrium experiments. For long enough hairpin and dimer oligonucleotides (yN greater than or equal to 24), in either native or denatured forms, we predict that the (positive) difference gamma infinity - gamma N increases linearly with increasing N-1. For smaller values of N the difference gamma infinity - gamma N continues to increase with increasing N-1.
盐浓度对寡核苷酸螺旋稳定性的影响,直接依据ΔγN→yN来分析,该值等同于γdenyN - γnatN,即变性状态(具有yN个磷酸电荷)与天然状态(具有N个磷酸电荷)的盐 - 核苷酸磷酸优先相互作用系数之差(发夹变性时y = 1,二聚体变性时y = 0.5)。先前对发夹寡核苷酸(18 < N < 44)变性的实验研究表明,ΔγN→N与Δγ∞之间存在显著差异,Δγ∞是相应多核苷酸变性所确定的值。这些差异是寡电解质末端效应的热力学表现。相比之下,关于寡核苷酸二聚体螺旋(N≤22)变性的现有数据表明,Δγ∞与ΔγN→0.5N之间的差异,进而寡电解质末端效应,很小或可忽略不计。为了确定这些关于寡电解质末端效应重要性的明显相互矛盾的暗示的根源,我们通过巨正则蒙特卡罗模拟计算了γN对N的依赖性,该模拟针对每个寡聚体构象的结构和电荷分布的理想化模型。我们的计算结果与d(TA)发夹寡核苷酸的实验发现定量一致,即随着N - 1增加,-ΔγN→N线性下降,并且与现有的ΔγN→0.5N的实验测定结果一致。这些结果说明了当将Δγ∞与短二聚体螺旋(N≤22)的ΔγN→0.5N值进行比较时,发夹变性数据所显示的大静电末端效应是如何被掩盖的。对于0.5N大于24的情况,预计 -ΔγN→0.5N是N - 1的线性函数,其斜率与 -ΔγN→N作为N - 1的函数的相应斜率符号相反,且对盐浓度的依赖性更强。我们的计算还得出了关于γN各个值对N的依赖性的预测,可通过膜透析平衡实验确定唐南系数来进行检验。对于足够长的发夹和二聚体寡核苷酸(yN≥24),无论是天然形式还是变性形式,我们预测(正)差异γ∞ - γN随着N - 1的增加而线性增加。对于较小的N值,差异γ∞ - γN继续随着N - 1的增加而增加。