Schwyzer R
Biochemistry. 1986 Jul 29;25(15):4281-6. doi: 10.1021/bi00363a016.
Equilibrium thermodynamic and kinetic estimations were used to confirm the rather unusual conformation, orientation, and accumulation of dynorphin A-(1-13)-tridecapeptide (dynorphin1-13) on the surface of neutral lipid membranes, as observed by Erne et al. [Erne, D., Sargent, D. F., & Schwyzer, R. (1985) Biochemistry 24, 4261-4263]. I started from the premise that the most stable conformation of molecularly disperse peptides in contact with the hydrophobic phase of a membrane is helical [Henderson, R. (1979) Soc. Gen. Physiol. Ser. 33, 3-15]. Calculation of the Gibbs free energy difference for the transfer of increasing numbers m of N-terminal residues of dynorphin1-13 from their random-coil conformation in water to their alpha-helical conformation in a hydrophobic phase, with the values provided by Von Heijne and Blomberg [Von Heijne, G., & Blomberg, C. (1979) Eur. J. Biochem. 97, 175-181], showed an energy minimum at m = 9 that corresponded to the observed apparent association constant of 9 X 10(4) L/mol. This confirmed our experimental observations. The orientation of dynorphin1-13 in the interphase was estimated by calculation of the molecular amphiphilic moment A. This force vector was defined in analogy to the "helical" and "structural" hydrophobic moments of Eisenberg et al. [Eisenberg, D., Weiss, R. M., & Terwilliger, T. C. (1982) Nature (London) 299, 371-374]. It takes into account the segregation of hydrophobic and hydrophilic residues with respect to the center of the alpha-helix. A peptide located in a hydrophobic-hydrophilic gradient experiences a torque that tends to orient A in a direction perpendicular to the surfaces of equal hydrophobicity.(ABSTRACT TRUNCATED AT 250 WORDS)
如厄内等人[厄内,D.,萨金特,D. F.,& 施维泽,R.(1985年)《生物化学》24卷,4261 - 4263页]所观察到的,采用平衡热力学和动力学估计来证实强啡肽A -(1 - 13)- 十三肽(强啡肽1 - 13)在中性脂质膜表面相当不寻常的构象、取向和聚集情况。我的出发点是,与膜的疏水相接触的分子分散肽的最稳定构象是螺旋构象[亨德森,R.(1979年)《普通生理学学会系列》33卷,3 - 15页]。利用冯·海涅和布洛姆贝格[冯·海涅,G.,& 布洛姆贝格,C.(1979年)《欧洲生物化学杂志》97卷,175 - 181页]提供的值,计算强啡肽1 - 13从其在水中的无规卷曲构象转变为在疏水相中的α - 螺旋构象时,N端残基数m增加时的吉布斯自由能差,结果显示在m = 9时能量最小,这与观察到的9×10⁴L/mol的表观缔合常数相对应。这证实了我们的实验观察结果。通过计算分子两亲矩A来估计强啡肽1 - 13在界面中的取向。这个力矢量是类似于艾森伯格等人[艾森伯格,D.,魏斯,R. M.,& 特威利格,T. C.(1982年)《自然(伦敦)》299卷,371 - 374页]的“螺旋”和“结构”疏水矩来定义的。它考虑了疏水和亲水残基相对于α - 螺旋中心的分隔情况。位于疏水 - 亲水梯度中的肽会受到一个扭矩,该扭矩倾向于使A沿垂直于等疏水性表面的方向取向。(摘要截断于250字)