computer modeling in molecular biology.pdf
computer modeling in molecular biology.pdf
computer modeling in molecular biology.pdf
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134 Benoft Roux6.1 IntroductionThe movement of ions across biological membranes is one of the most fundamentalprocess occurr<strong>in</strong>g <strong>in</strong> liv<strong>in</strong>g cells [l]. Without specific macro<strong>molecular</strong> structures,“ion channels”, the lipid membrane would present a prohibitively high energy barrierto the passage of any ion [2]. Selectivity for specific ions and a remarkably highrate of transport are key features of biological ion channels. For example, an averageof one hundred million Kf ions per second, selected over Na’ ions by a factor ofone hundred to one, can cross a frog node Delayed rectifier K channel underphysiological conditions [l]. Considerable efforts are now dedicated to the characterizationof ion permeation <strong>in</strong> <strong>molecular</strong> terms and to identify structural motifs thatcarry out specific functions. Advances due to the Patch Clamp technique [3] havepermitted the detection, at least on the millisecond time-scale, of the unitary eventsgovern<strong>in</strong>g the permeation of ions such as the open<strong>in</strong>g and the clos<strong>in</strong>g of a s<strong>in</strong>glemembrane channel. Primary am<strong>in</strong>o acid sequences have been deduced for severalbiological channel molecules and site-directed mutagenesis is used to identify the keyresidues <strong>in</strong>volved <strong>in</strong> the function of biological channels [4]. Recently, dramatic examplesshowed that mutation of a s<strong>in</strong>gle residue can alter the Na’ channel to aCaf2 permeable channel [5], and that a substitution of three am<strong>in</strong>o acids is able toconvert a cation-selective channel <strong>in</strong>to an anion-selective channel [6].The relation of structure to function <strong>in</strong> ion channels is of central concern forphysiologists. Results from biochemical dissection, site-directed mutagenesis, chemicalmodifications and ion-flux measurements are be<strong>in</strong>g used, <strong>in</strong> comb<strong>in</strong>ation withstructure prediction algorithms and <strong>molecular</strong> mechanics calculations, to determ<strong>in</strong>ethe overall topology and the three-dimensional structure of important biologicalchannels [4, 7- 111. Nevertheless, the relative <strong>in</strong>tractability of biological membraneprote<strong>in</strong>s still poses severe problems. Experimentally determ<strong>in</strong>ed structures withatomic resolution are available only for a few membrane prote<strong>in</strong>s : the photosyntheticreaction center [12], bacteriorhodops<strong>in</strong> [13], a por<strong>in</strong> from Rhodobacter capsulatus[14], and the OmpF and PhoE por<strong>in</strong>s of bacteria E. coli [15]; there is also some <strong>in</strong>formationabout the general macro<strong>molecular</strong> shape of the acetylchol<strong>in</strong>e receptor [16]and the fast Na’ channel [17] from high resolution electron microscopy. Membraneprote<strong>in</strong>s are difficult to characterize structurally, primarily because the requirementfor ma<strong>in</strong>ta<strong>in</strong><strong>in</strong>g a membrane environment h<strong>in</strong>ders purification and crystallizationand complicates spectroscopic measurements. The task is further complicated by thefact that biological ion channels are particularly complex multisubunits membraneprote<strong>in</strong>s. This is the reason why much of the progress <strong>in</strong> understand<strong>in</strong>g the relationof structure to function <strong>in</strong> ion channels has been ga<strong>in</strong>ed by study<strong>in</strong>g small artificialpore form<strong>in</strong>g molecules such as gramicid<strong>in</strong> A (Figure 6-1). This small pentadecapeptideforms a membrane channel that appears to be ideally selective for smallunivalent cations, while it is blocked by divalent cations, and impermeable to anions