Crystallographic structure of the K intermediate of bacteriorhodopsin: Conservation of free energy after photoisomerization of the retinal

被引:183
作者
Schobert, B
Cupp-Vickery, J
Hornak, V
Smith, SO
Lanyi, JK [1 ]
机构
[1] Univ Calif Irvine, Dept Phys & Biophys, Irvine, CA 92697 USA
[2] SUNY Stony Brook, Ctr Struct Biol, Stony Brook, NY 11794 USA
[3] Univ Calif Irvine, Dept Biochem & Cell Biol, Irvine, CA 92697 USA
基金
美国国家卫生研究院;
关键词
bacteriorhodopsin; retinal; K intermediate; photoisomerization; membrane proteins;
D O I
10.1016/S0022-2836(02)00681-2
中图分类号
Q5 [生物化学]; Q7 [分子生物学];
学科分类号
071010 ; 081704 ;
摘要
The K state, an early intermediate of the bacteriorhodopsin photocycle, contains the excess free energy used for light-driven proton transport. The energy gain must reside in or near the photoisomerized retinal, but in what form has long been an open question. We produced the K intermediate in bacteriorhodopsin crystals in a photostationary state at 100 K, with 40% yield, and determined its X-ray diffraction structure to 1.43 Angstrom resolution. In independent refinements of data from four crystals, the changes are confined mainly to the photoisomerized retinal. The retinal is 13-cis,15-anti, as known from vibrational spectroscopy. The C-13=C-14 bond is rotated nearly fully to cis from the initial trans configuration, but the C-14-C-15 and C-15=NZ bonds are partially counter-rotated. This strained geometry keeps the direction of the Schiff base N-H bond vector roughly in the extracellular direction, but the angle of its hydrogen bond with water 402, that connects it to the anionic Asp85 and Asp212, is not optimal. Weakening of this hydrogen bond may account for many of the reported features of the infrared spectrum of K, and for its photoelectric signal, as well as the deprotonation of the Schiff base later in the cycle. Importantly, although 13-cis, the retinal does not assume the expected bent shape of this configuration. Comparison of the calculated energy of the increased angle Of C-12-C-13=C-14, that allows this distortion, with the earlier reported calorimetric measurement of the enthalpy gain of the K state indicates that a significant part of the excess energy is conserved in the bond strain at C-13. (C) 2002 Elsevier Science Ltd. All rights reserved.
引用
收藏
页码:715 / 726
页数:12
相关论文
共 57 条
[1]   THE CCP4 SUITE - PROGRAMS FOR PROTEIN CRYSTALLOGRAPHY [J].
BAILEY, S .
ACTA CRYSTALLOGRAPHICA SECTION D-BIOLOGICAL CRYSTALLOGRAPHY, 1994, 50 :760-763
[2]  
Balashov SP, 2001, PHOTOCHEM PHOTOBIOL, V73, P453, DOI 10.1562/0031-8655(2001)073<0453:TASIOT>2.0.CO
[3]  
2
[4]   Protein, lipid and water organization in bacteriorhodopsin crystals:: a molecular view of the purple membrana at 1.9 Å resolution [J].
Belrhali, H ;
Nollert, P ;
Royant, A ;
Menzel, C ;
Rosenbusch, JP ;
Landau, EM ;
Pebay-Peyroula, E .
STRUCTURE, 1999, 7 (08) :909-917
[5]   ENERGY-STORAGE IN THE PRIMARY STEP OF THE PHOTOCYCLE OF BACTERIORHODOPSIN [J].
BIRGE, RR ;
COOPER, TM .
BIOPHYSICAL JOURNAL, 1983, 42 (01) :61-69
[6]   REVISED ASSIGNMENT OF ENERGY-STORAGE IN THE PRIMARY PHOTOCHEMICAL EVENT IN BACTERIORHODOPSIN [J].
BIRGE, RR ;
COOPER, TM ;
LAWRENCE, AF ;
MASTHAY, MB ;
ZHANG, CF ;
ZIDOVETZKI, R .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 1991, 113 (11) :4327-4328
[7]   RESONANCE RAMAN-SPECTRA OF BACTERIORHODOPSINS PRIMARY PHOTOPRODUCT - EVIDENCE FOR A DISTORTED 13-CIS RETINAL CHROMOPHORE [J].
BRAIMAN, M ;
MATHIES, R .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA-BIOLOGICAL SCIENCES, 1982, 79 (02) :403-407
[8]   The projection structure of the low temperature K intermediate of the bacteriorhodopsin photocycle determined by electron diffraction [J].
Bulllough, PA ;
Henderson, R .
JOURNAL OF MOLECULAR BIOLOGY, 1999, 286 (05) :1663-1671
[9]  
CHAMOROVSKY SK, 1987, BIOFIZIKA+, V32, P601
[10]   Partitioning of free energy gain between the photoisomerized retinal and the protein in bacteriorhodopsin [J].
Dioumaev, AK ;
Brown, LS ;
Needleman, R ;
Lanyi, JK .
BIOCHEMISTRY, 1998, 37 (28) :9889-9893