F. L. Suddath

Three-dimensional tertiary structure of yeast phenylalanine transfer RNA

The 3-angstrom electron density map of crystalline yeast phenylalanine transfer RNA has provided us with a complete three-dimensional model which defines the positions of all of the nucleotide residues in the moleclule. The overall features of the molecule are virtually the same as those seen at a resolution of 4 angstroms except that many additional details of tertiary structure are now visualized. Ten types of hydrogen bonding are identified which define the specificity of tertiary interactions. The molecule is also stabilized by considerable stacking of the planar purines and pyrimidines. This tertiary structure explains, in a simple and direct fashion, chemical modification studies of transfer RNA. Since most of the tertiary interactions involve nucleotides which are common to all transfer RNA s, it is likely that this three-dimensional structure provides a basic pattern of folding which may help to clarify the three-dimensional structure of all transfer RNAs.

RNA double-helical fragments at atomic resolution: I. The crystal and molecular structure of sodium adenylyl-3′,5′-uridine hexahydrate☆

Abstract The crystal structure of sodium adenylyl-3′,5′-uridine (ApU) hexahydrate has been determined by X-ray diffraction procedures and refined to an R factor of 0.057. ApU crystallizes with two molecules per asymmetric unit in a monoclinic unit cell, space group P21, with cell dimensions: a = 18.025, b = 17.501, c = 9.677 A and β = 99.45 ° . The two independent molecules of ApU form a small segment of right-handed antiparallel double-helical RNA in the crystal, with Watson-Crick base-pairing between adenine and uracil. This is the first time that this Watson-Crick base-pair has been seen unambiguously at atomic resolution and it is also the first time that a nucleic acid fragment with double-helical symmetry has been seen at atomic resolution. The distance between the C1′ atoma of the adenine-uracil base-pair is slightly shorter than the analogous distance seen in guanine-cytosine base-pairs. The bases in each strand are heavily stacked. One sodium cation binds to the phosphates, as expected; however, the other sodium cation binds on the dyad axis in the minor groove of the double helix. It is co-ordinated directly to the two uracil carbonyl groups which protrude into the minor groove and is shielded from the nearest phosphates by a shell of water. This binding appears to be sequence-specific for ApU. One of the adenines also forms a pair of hydrogen bonds to a nearby ribose, utilizing N6 and N7. The 12 water molecules per double-helical fragment are all part of the first co-ordination shell. The ions and the symmetry of the double-helical fragment are the major organizing elements of the solvent region.

Three-Dimensional Structure of Yeast Phenylalanine Transfer RNA: Folding of the Polynucleotide Chain

At 4 � resolution the polynucleotides in yeast phenylalanine transfer RNA are seen in a series of electron dense masses about 5.8 � apart. These peaks are probably associated with the phosphate groups, while lower levels of electron density between segments of adjacent polynucleotide chains are interpreted as arising from hydrogen-bonded purine-pyrimidine base pairs. It is possible to trace the entire polynucleotide chain with only two minor regions of ambiguity. The polynucleotide chain has a secondary structure consistent with the cloverleaf conformation; however, its folding is different from that proposed in any model. The molecule is made of two double-stranded helical regions oriented at right angles to each other in the shape of an L. One end of the L has the CCA acceptor; the anticodon loop is at the other end, and the dihydrouridine and TψC loops form the corner.

X-ray crystallographic studies of polymorphic forms of yeast phenylalanine transfer RNA

Abstract Yeast phenylalanine transfer RNA has been found to crystallize in five different crystal systems involving eight different space groups. The X-ray diffraction characteristics of these forms are described. One of the orthorhombic forms yields a diffraction pattern with higher resolution than either the hexagonal, the cubic or the monoclinic forms. One region of this orthorhombic diffraction pattern is particularly sensitive to X-ray exposure and to changes in the concentration of various solutes. The diffraction pattern from the cubic crystal form extends to a resolution of 3 A, and there are a number of strong reflections in the 3 to 4 A region which suggest that double-helical segments of the tRNA molecules are oriented along the 4-fold axes. Some comments are made regarding the nature of the polymorphism in the transfer RNA crystals.

Unit cell transformations in yeast phenylalanine transfer RNA crystals

Abstract The orthorhombic unit cell of crystalline yeast phenylalanine transfer RNA has dimensions a = 33 A , b = 56 A and c = 161 A . When the mother liquor dries partially, a series of transformations takes place in which the a and b axes change very little but the c axis decreases abruptly first to 128 A and then to 109 A. In a closely related orthorhombic cell in a different space group the c axis is 104 A. Although there is some loss in resolution in these smaller unit cells, the over-all distribution of scattering intensity does not change substantially. This suggests that the tRNA molecules can slide together along the c axis without a substantial change in internal structure.