Rayan Gamal, Macgregor Robert B
Department of Pharmaceutical Sciences, Leslie Dan Faculty of Pharmacy, University of Toronto, 19 Russell Street, Toronto, Ontario M5S 2S2, Canada.
J Phys Chem B. 2005 Aug 18;109(32):15558-65. doi: 10.1021/jp050899c.
The helix-coil transition of poly[d(I-C)] and poly[d(A-T)] was studied as a function of hydrostatic pressure, temperature, and sodium ion concentration. These studies were undertaken in light of a recently published phase diagram for double stranded nucleic acids [Dubins et al. J. Am. Chem. Soc. 2001, 123, 9254-9259]. The sign and magnitude of the volume change for the heat-induced helix-coil transition, DeltaV(T), of poly[d(I-C)] and poly[d(A-T)] were dependent on the helix-coil transition temperature, T(M), at atmospheric pressure. The sign of DeltaV(T) changed from negative to positive as T(M) was increased by increasing the sodium ion concentration. For poly[d(I-C)], DeltaV(T) = 0 cm(3) mol(-1), when the sodium ion concentration is such that the spectroscopically monitored T(M) = 55 degrees C at atmospheric pressure. For poly[d(A-T)], the value of DeltaV(T) = 0 under conditions such that T(M) = 47 degrees C at atmospheric pressure. Negative values of DeltaV(T) imply that the helical form is destabilized at high pressure. Under experimental conditions where the DeltaV(T) for the transition is negative, the transition could be caused by increasing the pressure under isothermal conditions. At temperatures below T(M) measured at atmospheric pressure the midpoint of the pressure-induced helix-coil transition, P(M), decreases with increasing temperature. The volume change of the pressure-induced transitions helix-coil transition, DeltaV(P), was calculated assuming a two-state model. The magnitude of DeltaV(P) (per cooperative length) was much larger than the volume change (per base pair) measured for the heat-induced transition, DeltaV(T), calculated using the Clapeyron equation. The ratio of these two volume changes was used to calculate the cooperative length for the pressure-induced transition. This parameter depends strongly on temperature, becoming greater closer to T(M) measured at atmospheric pressure. At temperatures approaching T(M) the magnitude of the cooperative length of the pressure-induced transition is approximately twice that observed for the heat-induced transition (N(T)). On the basis of the temperature dependence of the DeltaV(T) for the two polymers the coefficient of thermal expansion of the two polymers was found to be 0.17 and 0.16 cm(3) K(-1) mol(-1) for poly[d(I-C)] and poly[d(A-T)], respectively.
研究了聚[d(I-C)]和聚[d(A-T)]的螺旋-卷曲转变与静水压力、温度和钠离子浓度的关系。这些研究是根据最近发表的双链核酸相图[杜宾斯等人,《美国化学会志》,2001年,123卷,9254 - 9259页]进行的。聚[d(I-C)]和聚[d(A-T)]热诱导螺旋-卷曲转变的体积变化ΔV(T)的符号和大小取决于常压下的螺旋-卷曲转变温度T(M)。随着钠离子浓度增加导致T(M)升高,ΔV(T)的符号从负变为正。对于聚[d(I-C)],当钠离子浓度使得常压下光谱监测的T(M) = 55℃时,ΔV(T) = 0 cm³ mol⁻¹。对于聚[d(A-T)],在常压下T(M) = 47℃的条件下,ΔV(T)的值为0。ΔV(T)为负值意味着螺旋形式在高压下不稳定。在转变的ΔV(T)为负的实验条件下,转变可通过在等温条件下增加压力来引起。在低于常压下测量的T(M)的温度下,压力诱导的螺旋-卷曲转变的中点P(M)随温度升高而降低。假设为二态模型计算压力诱导的螺旋-卷曲转变的体积变化ΔV(P)。ΔV(P)(每协同长度)的大小远大于使用克拉佩龙方程计算的热诱导转变的体积变化(每碱基对)ΔV(T)。这两个体积变化的比值用于计算压力诱导转变的协同长度。该参数强烈依赖于温度,在接近常压下测量的T(M)时变得更大。在接近T(M)的温度下,压力诱导转变的协同长度大小约为热诱导转变(N(T))观察值的两倍。基于两种聚合物的ΔV(T)对温度的依赖性,发现聚[d(I-C)]和聚[d(A-T)]的热膨胀系数分别为0.17和0.16 cm³ K⁻¹ mol⁻¹。