Nechipurenko Y D, Gursky G V
Biophys Chem. 1986 Aug;24(3):195-209. doi: 10.1016/0301-4622(86)85025-6.
Equations are derived for description of cooperative binding of large ligands to a homogeneous polynucleotide lattice for a wide variety of binding models. Both short- and long-range interactions between nearest-neighbour bound ligands are taken into account. It is shown that cooperative binding of ligand at high levels of occupancy can be described with good accuracy by the equation derived for the noncooperative binding of the same ligand with an apparent binding constant Keff. A new method is proposed for the analysis of cooperative binding isotherms. It is based on a comparison of the asymptotic behavior of cooperative and noncooperative binding isotherms in the limit when the occupancy of lattice by ligand approaches the saturation level of binding. It is demonstrated that cooperative effects mediated by direct contact between bound ligands can be divided into two classes depending on whether dimeric species or aggregates of unrestricted size are formed by bound ligands on the lattice at high levels of occupancy. These two classes can be easily distinguished on strictly empirical grounds. In particular, if interligand interactions favor the formation of dimeric species on DNA, Keff approximately a 1/2 where a is the interligand interaction constant. If interligand interactions generate aggregates of unrestricted size, Keff approximately aL + 1 where L is the size of binding site for the ligand on DNA. We also demonstrate that cooperative systems in which interligand interaction extends over two or more free polymer residues can be distinguished from systems in which only short-range interactions mediated by direct contacts between bound ligands are allowed.
针对多种结合模型,推导了用于描述大配体与均匀多核苷酸晶格协同结合的方程。考虑了最近邻结合配体之间的短程和长程相互作用。结果表明,在高占据水平下配体的协同结合可以用为相同配体的非协同结合推导的方程以较高精度描述,该方程具有表观结合常数Keff。提出了一种分析协同结合等温线的新方法。它基于在配体对晶格的占据接近结合饱和水平的极限情况下,比较协同和非协同结合等温线的渐近行为。结果表明,由结合配体之间的直接接触介导的协同效应可分为两类,这取决于在高占据水平下晶格上的结合配体是形成二聚体物种还是无限制大小的聚集体。这两类可以很容易地基于严格的经验依据区分开来。特别是,如果配体间相互作用有利于在DNA上形成二聚体物种,则Keff约为a的1/2,其中a是配体间相互作用常数。如果配体间相互作用产生无限制大小的聚集体,则Keff约为aL + 1,其中L是配体在DNA上结合位点的大小。我们还证明,配体间相互作用延伸到两个或更多个自由聚合物残基的协同系统可以与仅允许由结合配体之间的直接接触介导的短程相互作用的系统区分开来。