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马盖宁2酰胺与脂质膜的相互作用:肽结合和孔形成的量热法检测

Magainin 2 amide interaction with lipid membranes: calorimetric detection of peptide binding and pore formation.

作者信息

Wenk M R, Seelig J

机构信息

Department of Biophysical Chemistry, Biocenter of the University of Basel, Switzerland.

出版信息

Biochemistry. 1998 Mar 17;37(11):3909-16. doi: 10.1021/bi972615n.

DOI:10.1021/bi972615n
PMID:9521712
Abstract

The interaction of the antibiotic magainin 2 amide (M2a) with lipid bilayers was investigated with high-sensitivity titration calorimetry. The enthalpy of transfer of the cationic M2a to negatively charged small unilamellar vesicles composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) and 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoglycerol (POPG) (75:25, mol/mol) was measured as delta H = -17.0 +/- 1 kcal/mol of peptide. The adsorption isotherm was determined by injecting lipid vesicles into peptide solutions at low peptide concentrations (cPo < 7 microM). The apparent partition coefficient was Kapp approximately 1.2 x 10(4) M-1 at a peptide equilibrium concentration of 1 microM but decreased with increasing peptide concentration. The hydrophobic partitioning of M2a into the lipid membrane is modulated by electrostatic effects that arise from the attraction of the positively charged peptide to the negatively charged membrane. Using the Gouy-Chapman theory to correct for electrostatic attraction, the experimental binding isotherms can be explained with an intrinsic (hydrophobic) partition coefficient of K = 55 +/- 5 M-1 and an effective peptide charge of z = 3.7-3.8. The free energy of binding is delta G = -4.8 kcal/mol. At peptide concentrations cPo > approximately 7 microM, a second effect comes into play, and the titration enthalpies can no longer be explained exclusively by peptide partitioning. The first few injections produce enthalpies of reaction which are distinctly smaller than expected from a pure partition equilibrium, followed by a series of injections with reaction heats larger than expected. After subtracting the enthalpic contribution due to partitioning, the residual enthalpies are endothermic for the first few injections, and exothermic for the consecutive steps. Furthermore, the endothermic excess heat is compensated exactly by the exothermic excess heat; i.e., the excess heat consumed in the first part of the titration experiment is returned during the second part. Endothermic excess enthalpies are observed for total molar peptide-to-lipid ratios of P/L > approximately 3.0%, whereas exothermic excess heats were seen for 0.7% < P/L < 3.0%. Below P/L < approximately 0.7%, the binding follows the partition equilibrium. Based on earlier spectroscopic evidence, it is suggested that magainin 2 amide binds to the lipid membrane and forms pores at high peptide-to-lipid ratio, this process being characterized by an endothermic reaction enthalpy. Pore formation is reversed with increasing lipid concentration, and the peptide pores disintegrate. The limiting peptide-to-lipid ratio deduced from titration calorimetry for M2a pore formation is in excellent agreement with spectroscopic methods. The enthalpy of pore formation amounts to delta H = +6.2 +/- 1.6 kcal/mol peptide or delta H approximately 25-45 kcal/mol pore if the pore is comprised of 4-7 peptide molecules.

摘要

采用高灵敏度滴定热分析法研究了抗生素马盖宁2酰胺(M2a)与脂质双层的相互作用。测定了阳离子型M2a转移至由1-棕榈酰-2-油酰-sn-甘油-3-磷酸胆碱(POPC)和1-棕榈酰-2-油酰-sn-甘油-3-磷酸甘油(POPG)(75:25,摩尔/摩尔)组成的带负电荷的小单层囊泡的焓变,为ΔH = -17.0±1千卡/摩尔肽。吸附等温线通过在低肽浓度(cPo < 7 μM)下将脂质囊泡注入肽溶液来测定。在肽平衡浓度为1 μM时,表观分配系数Kapp约为1.2×10⁴ M⁻¹,但随肽浓度增加而降低。M2a向脂质膜的疏水分配受到静电效应的调节,这种静电效应源于带正电荷的肽与带负电荷的膜之间的吸引力。利用古依-查普曼理论校正静电吸引力后,实验结合等温线可用内在(疏水)分配系数K = 55±5 M⁻¹和有效肽电荷z = 3.7 - 3.8来解释。结合自由能为ΔG = -4.8千卡/摩尔。在肽浓度cPo > 约7 μM时,第二种效应开始起作用,滴定焓不再能仅由肽分配来解释。最初几次注射产生的反应焓明显小于纯分配平衡预期的值,随后一系列注射的反应热大于预期值。减去由于分配引起的焓贡献后,最初几次注射的残余焓是吸热的,而连续步骤是放热的。此外,吸热的多余热量正好被放热的多余热量补偿;即,滴定实验第一部分消耗的多余热量在第二部分返回。当总摩尔肽与脂质比P/L > 约3.0%时观察到吸热的多余焓,而当0.7% < P/L < 3.0%时观察到放热的多余热量。在P/L < 约0.7%时,结合遵循分配平衡。基于早期的光谱证据,有人提出马盖宁2酰胺与脂质膜结合并在高肽与脂质比时形成孔,这个过程的特征是吸热反应焓。随着脂质浓度增加,孔形成逆转,肽孔解体。通过滴定热分析法推导的M2a孔形成的极限肽与脂质比与光谱方法非常一致。孔形成的焓为ΔH = +6.2±1.6千卡/摩尔肽,或者如果孔由4 - 7个肽分子组成,则ΔH约为25 - 45千卡/摩尔孔。

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