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嗜热栖热菌磷酸甘油酸激酶及其分离结构域的热力学研究:通过差示扫描量热法和圆二色光谱监测可逆热解折叠

Thermodynamic study of phosphoglycerate kinase from Thermotoga maritima and its isolated domains: reversible thermal unfolding monitored by differential scanning calorimetry and circular dichroism spectroscopy.

作者信息

Zaiss K, Jaenicke R

机构信息

Institut für Biophysik und Physikalische Biochemie, Universität Regensburg, Germany.

出版信息

Biochemistry. 1999 Apr 6;38(14):4633-9. doi: 10.1021/bi982447e.

DOI:10.1021/bi982447e
PMID:10194385
Abstract

The folding of phosphoglycerate kinase (PGK) from the hyperthermophilic bacterium Thermotoga maritima and its isolated N- and C-terminal domains (N1/2 and C1/2) was characterized by differential scanning calorimetry (DSC) and circular dichroism (CD) spectroscopy. At pH 3.0-4.0, reversible thermal denaturation of TmPGK occurred below 90 degrees C. The corresponding peaks in the partial molar heat capacity function were fitted by a four-state model, describing three well-defined unfolding transitions. Using CD spectroscopy, these are ascribed to the disruption of the domain interactions and subsequent sequential unfolding of the two domains. The isolated N-terminal domain unfolds reversibly between pH 3.0 and pH 4.0 to >90% and at pH 7.0 to about 70%. In contrast, the isolated engineered C-terminal domain only shows reversible thermal denaturation between pH 3.0 and pH 3.5. Neither N1/2 nor C1/2 obeys the simple two-state mechanism of unfolding. Instead, both unfold via a partially structured intermediate. In the case of N1/2, the intermediate exhibits native secondary structure and perturbed tertiary structure, whereas for C1/2 the intermediate could not be defined with certainty.

摘要

对嗜热栖热菌磷酸甘油酸激酶(PGK)及其分离出的N端和C端结构域(N1/2和C1/2)进行了差示扫描量热法(DSC)和圆二色性(CD)光谱表征。在pH 3.0 - 4.0时,嗜热栖热菌PGK(TmPGK)在90℃以下发生可逆热变性。部分摩尔热容函数中的相应峰通过四态模型拟合,该模型描述了三个明确的解折叠转变。利用CD光谱,这些转变归因于结构域间相互作用的破坏以及随后两个结构域的顺序解折叠。分离出的N端结构域在pH 3.0至pH 4.0之间可逆解折叠至>90%,在pH 7.0时解折叠至约70%。相比之下,分离出的工程化C端结构域仅在pH 3.0至pH 3.5之间显示可逆热变性。N1/2和C1/2均不遵循简单的两态解折叠机制。相反,两者均通过部分结构化中间体解折叠。在N1/2的情况下,中间体呈现天然二级结构和受扰三级结构,而对于C1/2,中间体无法明确界定。

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