PubMed · 9671285
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P Campbell. 1998-07-09. New policy for structure data.. https://doi.org/10.1038/27971
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We describe the three-dimensional structure of higher plant photosystem I (PSI) as obtained by electron microscopy of two-dimensional crystals formed at the grana margins of thylakoid membranes. The negatively stained crystalline areas displayed unit cell dimensions a = 26.6 nm, b = 27.7 nm, and gamma = 90(o), and p22121 plane group symmetry consisting of two monomers facing upward and two monomers facing downward with respect to the membrane plane. Higher plant PSI shows several structural similarities to the cyanobacterial PSI complex, with a prominent ridge on the stromal side of the complex. The stromal ridge is resolved into at least three separate domains that are interpreted as representing the three well characterized stromal subunits, the psa C, D, and E gene products. The lumenal surface is relatively flat but exhibits a distinct central depression that may be the binding site for plastocyanin. Higher plant PSI is of dimensions 15-16 x 11-12.5 nm, and thus leaves a larger footprint in the membrane than its cyanobacterial equivalent (13 x 10.5 nm). It is expected that additional membrane-bound polypeptides will be present in the higher plant PSI. Both higher plant and cyanobacterial complexes span about 8-9 nm in the direction orthogonal to the membrane. This report represents the first three-dimensional structure for the higher plant PSI complex.
Liquid crystalline solutions of Pluronic copolymers are versatile alternatives to solutions of entangled, random coil polymers as replaceable media for capillary gel electrophoresis (CGE). Pluronic copolymers are tri-block polymers of poly(ethylene oxide) [(EO)x] and poly(propylene oxide) [(PO)y] with the general formula (EO)x(PO)y(EO)x. Large micelles form in aqueous solutions in which central, hydrophobic cores of (PO)y segments are surrounded by "brushes" of hydrated (EO)x tails. Solutions of Pluronic F127 (BASF Performance Chemicals) in a concentration range of about 18-30% are liquids at refrigerator temperatures (< or = 5 degrees C) and are easily introduced into capillaries. A self-supporting, gel-like liquid crystalline phase is formed as the temperature is raised to > or = 20 degrees C. This liquid crystalline phase consists of spherical micelles with diameters of 17-18 nm which pack with local cubic symmetry. CGE in Pluronic F127 liquid crystals separates species within several chemical classes as varied as nucleoside monophosphates and organic dyes, oligonucleotides of 4-60 nucleotides, DNA fragments of 50-3000 base pairs (bp), and supercoiled plasmid DNAs of 2000-10,000 bp. Mechanisms of molecular sieving in polymer liquid crystals must differ in fundamental ways from separations in random polymer gels because molecules move around uncrosslinked obstacles that are larger than the smallest dimensions of typical analytes. Molecular sieving in Pluronic liquid crystals is envisioned to occur as molecules squeeze between hydrated (EO)x strands of micelle brushes, or through brushtips and interstitial spaces between micelles. Small molecules such as nucleotides appear to separate by a different mechanism involving partitioning between hydrophilic and hydrophobic environments. This process is termed "hydrophobic interaction electrophoresis". The unique structures of Pluronic copolymers and their liquid crystalline phases provide new challenges and opportunities in separations science.
The behaviour of amino acid side-chains in proteins in solution has been characterised by analysing NMR 3JHalphaH beta coupling constants and crystallographic chi1 torsion angles. Side-chains both in the core of native folded proteins and in situations where there is an absence of close packing including the random coil state have been considered. An analysis of experimental 3JHalphaH beta coupling constant data for ten proteins shows that in the core of native proteins a very close similarity is observed between the chi1 conformations adopted in solution and in crystals. There is clear evidence, however, for significant motional averaging about the chi1 torsion angles in solution. Using a model of a Gaussian distribution about the average torsion angles the extent of these fluctuations has been quantified; the standard deviation for the motion is 26 degrees, the fluctuations about chi1 in the protein core being similar in size to those found for main-chain phi torsion angles in solution. From the distribution of chi1 torsion angles in a data base of protein crystal structures, torsion angle populations and coupling constants have been predicted for a random coil polypeptide. Significant variations in the chi1 distributions for different amino acids give differences in the predicted coupling constants; for 3JHalphaH beta, for example, values of 5.1 and 5.7 Hz are predicted for serine compared with 4.9 and 9.9 Hz for leucine. Experimental data for short unstructured peptides show an excellent agreement with the predictions, indicating that the overall chi1 distributions in protein crystals reflect the local preferences of the amino acids. Predictions from the protein data base therefore provide an important framework for interpreting experimental data for non-native protein conformations and for residues on the surface of folded proteins.