Fixed target matrix for femtosecond time-resolved and in situ serial micro-crystallography.

We present a crystallography chip enabling in situ room temperature crystallography at microfocus synchrotron beamlines and X-ray free-electron laser (X-FEL) sources. Compared to other in situ approaches, we observe extremely low background and high diffraction data quality. The chip design is robust and allows fast and efficient loading of thousands of small crystals. The ability to load a large number of protein crystals, at room temperature and with high efficiency, into prescribed positions enables high throughput automated serial crystallography with microfocus synchrotron beamlines. In addition, we demonstrate the application of this chip for femtosecond time-resolved serial crystallography at the Linac Coherent Light Source (LCLS, Menlo Park, California, USA). The chip concept enables multiple images to be acquired from each crystal, allowing differential detection of changes in diffraction intensities in order to obtain high signal-to-noise and fully exploit the time resolution capabilities of XFELs.

Ligand pathways in myoglobin: a review of Trp cavity mutations.

The pathways for ligand entry and exit in myoglobin have now been well established by a wide variety of experimental results, including pico- to nano- to microsecond transient absorbance measurements and time-resolved X-ray crystallographic measurements. Trp insertions have been used to block, one at a time, the three major cavities occupied by photodissociated ligands. In this work, we review the effects of the L29(B10)W mutation, which places a large indole ring in the initial 'docking site' for photodissociated ligands. Then, the effects of blocking the Xe4 site with I28W, V68W, and I107W mutations and the Xe1 cavity with L89W, L104W, and F138W mutations are described. The structures of four of these mutants are shown for the first time (Trp28, Trp68, Trp107, and Trp 138 sperm whale metMb). All available results support a 'side path' mechanism in which ligands move into and out of myoglobin by outward rotation of the HisE7 side chain, but after entry can migrate into internal cavities, including the distal Xe4 and proximal Xe1 binding sites. The distal cavities act like the pocket of a baseball glove, catching the ligand and holding it long enough for the histidine gate to close and facilitate internal coordination with the heme iron atom. The physiological role of the proximal Xe1 site is less clear because changes in the size of this cavity have minimal effects on overall O(2) binding parameters.

Crystallographic analysis of two site-directed mutants of Azotobacter vinelandii ferredoxin.

The crystal structure of the C24A mutant of Azotobacter vinelandii 7Fe ferredoxin (FdI) has been solved and refined at 2.0-A resolution. The structure is isomorphous to native FdI except at the site of mutation where A24 moves toward the [4Fe-4S] cluster. In spite of this inefficient packing results: three of five van der Waals contacts from the S gamma of C24 in native FdI are lost and the remaining two become longer. Consequently, the [4Fe-4S] cluster is either disordered or has a higher temperature factor (B factor) compared to the rest of the C24A FdI molecule. In addition, the entire C24A FdI structure has a higher overall B factor than native FdI. Therefore, in comparison to native FdI, the C24A mutant is isomorphous but exhibits large differences in B factor, especially at the [4Fe-4S] cluster. In contrast, the C20A FdI structure (Martin, A. G., Burgess, B. K., Stout, C. D., Cash, V. L., Dean, D. R., Jensen, G. M., and Stephens, P. J. (1990) Proc. Natl. Acad. Sci. U. S. A. 87, 598-602), which contains large structural rearrangements in the vicinity of the [4Fe-4S] cluster, exhibits essentially no change in B factor. The conformational change observed at residue 24 is similar in both C24A and C20A FdI structures. The solvent accessibility of the Fe atoms in the [3Fe-4S] and [4Fe-4S] clusters is similar in C24A, C20A, and native FdI.

X-ray studies on crystalline complexes involving amino acids and peptides. Part XX. Crystal structures of DL-arginine acetate monohydrate and DL-lysine acetate and a comparison with the corresponding L-amino acid complexes.

Crystals of DL-arginine acetate monohydrate, C6H15N4O2+C2H3O2-.H2O, are monoclinic, P2(1)/c, with a = 13.552(2), b = 5.048(2), c = 18.837(3) A, beta = 101.34(2) degrees and Z = 4, and those of DL-lysine acetate, C6H15N2O2+.C2H3O2- are triclinic, P1, with a = 5.471(2), b = 7.656(2), c = 12.841(2) A, alpha = 94.48(1), beta = 94.59(2), gamma = 98.83(2) degrees and Z = 2. The structures have been solved by direct methods and refined to R = 0.058 and 0.077 for 1522 and 1259 observed reflections respectively. The difference in the number and the nature of proton donors leads to a difference in hydrogen bond density in the two structures. The basic elements of aggregation in both the structures are pairs of amino acid molecules, each pair stabilized by two centrosymmetrically related hydrogen bonds involving alpha-amino and alpha-carboxylate groups, stacked along the shortest dimension to form columns. The pairs are held together in each column by head-to-tail sequences. The columns stack along a crystallographic axis to form layers. Adjacent layers are bridged by acetate ions. The amino acid-acetate interactions are primarily through side chains and involve specific interactions and characteristic interaction patterns. The gross features of molecular aggregation are nearly the same in DL-arginine acetate monohydrate and L-arginine acetate whereas they are substantially different in the lysine complexes. In both cases, one of the two head-to-tail sequences in the L complex is replaced by a hydrogen bonded loop involving alpha-amino and alpha-carboxylate groups, in the DL complex. This may have implications for prebiotic condensation during chemical evolution.

X-ray studies on crystalline complexes involving amino acids and peptides. XV. Crystal structures of L-lysine D-glutamate and L-lysine D-aspartate monohydrate and the effect of chirality on molecular aggregation.

L-Lysine D-glutamate crystallizes in the monoclinic space group P2(1) with a = 4.902, b = 30.719, c = 9.679 A, beta = 90 degrees and Z = 4. The crystals of L-lysine D-aspartate monohydrate belong to the orthorhombic space group P2(1)2(1)2(1) with a = 5.458, b = 7.152, c = 36.022 A and Z = 4. The structures were solved by the direct methods and refined to R values of 0.125 and 0.040 respectively for 1412 and 1503 observed reflections. The glutamate complex is highly pseudosymmetric. The lysine molecules in it assume a conformation with the side chain staggered between the alpha-amino and the alpha-carboxylate groups. The interactions of the side chain amino groups of lysine in the two complexes are such that they form infinite sequences containing alternating amino and carboxylate groups. The molecular aggregation in the glutamate complex is very similar to that observed in L-arginine D-aspartate and L-arginine D-glutamate trihydrate, with the formation of double layers consisting of both types of molecules. In contrast to the situation in the other three LD complexes, the unlike molecules in L-lysine D-aspartate monohydrate aggregate into alternating layers as in the case of most LL complexes. The arrangement of molecules in the lysine layer is nearly the same as in L-lysine L-aspartate, with head-to-tail sequences as the central feature. The arrangement of aspartate ions in the layers containing them is, however, somewhat unusual. Thus the comparison between the LL and the LD complexes analyzed so far indicates that the reversal of chirality of one of the components in a complex leads to profound changes in molecular aggregation, but these changes could be of more than one type.