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Ravi Mahadeva, Wun-Shaing W. Chang, Timothy R. Dafforn, Diana J. Oakley, Richard C. Foreman, Jacqueline Calvin, Derek G.D. Wight, David A. Lomas
Published in Volume 103, Issue 7
J Clin Invest. 1999; 103(7):999–1006 doi:10.1172/JCI4874
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Figure 7

(a) The crystal structures of α1-antitrypsin (32, 33) demonstrated the availability of 232Cys and the position of the I (39Arg→Cys) mutation in helix A at the back of the molecule. The reactive center loop is shown in red; the A β-sheet, which must open to allow polymer formation, is illustrated in green. S α1-antitrypsin mediates its effect by breaking a hydrogen bond with 38Tyr in the shutter domain (20), which controls A β-sheet mobility. (b) Reactive loop/A-sheet polymerization with an open helical conformation (32) places the cysteine residues over 60 Å apart (right), but a closed helical conformation predictably brings the cysteine residues of different α1-antitrypsin molecules close to each other and therefore available for resonance energy transfer (left). In this model, the α1-antitrypsin molecules are ordered blue, green, and red (from bottom to top), with RET predictably occurring between the labeled cysteines of molecules of the same color.