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Biomedical subjects

B Senger

Publications and source records attributed to B Senger.

At least 37 records · Page 2Linked to original sources

The modified wobble base inosine in yeast tRNAIle is a positive determinant for aminoacylation by isoleucyl-tRNA synthetase.

Earlier work by two independent groups has established the fact that anticodons GAU and LAU of Escherichia coli tRNAIle isoacceptors play a critical role in the tRNA identity. Yeast possesses two isoleucine transfer RNAs, a major one with anticodon IAU and a minor one with anticodon PsiAPsi which are derived from the post-transcriptional modification of AAU and UAU gene sequences, respectively. We present direct evidence which reveals that inosine is a positive determinant for yeast isoleucyl-tRNA synthetase. We also show that yeast tRNAMet with guanosine at the wobble position becomes aminoacylated with isoleucine while methionine acceptance is lost. As inosine and guanosine share the 6-keto and the N-1 hydrogen groups, this suggests that these hydrogen donor and acceptor groups are determinants for isoleucine specificity. The role of the minor tRNAIle anticodon pseudouridines in tRNA isoleucylation could not be tested directly but was deduced from a 40-fold decrease in the activity of the unmodified transcript. The presence of the NHCO structure in guanosine, inosine, pseudouridine, and lysidine suggests a unifying model of wobble base recognition by the yeast and E. coli isoleucyl-tRNA synthetase. In contrast to lysidine which switches the identity of the tRNA from methionine to isoleucine [Muramatsu, T., Nishikawa, K., Nemoto, F., Kuchino, Y., Nishimura, S., Miyazawa, T., & Yokoyama, S. (1988) Nature 336, 179-181], pseudouridine-34 does not modify the specificity of the yeast minor tRNAIle since U-34 is a strong negative determinant for yeast MetRS. Therefore, the major role of Psi-34 (in combination with Psi-36 or not) is likely in isoleucine AUA codon specificity and translational fidelity.

Acylation↗

Influence of different parameters on bone heating and drilling time in implantology.

The influence of various parameters on bone heating during drilling and drilling time was studied in vitro in a bovine cortical femur model. Drilling using a standard, a surgical or a laboratory motor unit did not affect bone temperature elevation. For a given speed, low 1/40 reduction contra-angle was more effective in moderating temperature elevation when compared to 1/10 reduction; but drilling time in this case (1/40) had to be doubled. Enhancing the drilling load from 0.8 kg to 2 kg had little effect on temperature elevation at 400 rpm and 800 rpm (< 3 degrees C). Drilling time drastically decreased and was inversely proportional to the square of the load. Predrilling did not affect temperature elevation, but decreased drilling time. From 400 rpm to 10,000 rpm, temperature elevation was positively correlated with drilling speed. It further decreased up to 24,000 rpm and then was constant up to 40,000 rpm. Drilling time was proportionally reduced with increased rotation speed. Strikingly, heat was largely dissipated within 10 s at high rotation speed. The use of a cryogenic spray at 24,000 rpm allowed the reduction of temperature elevation. Finally, protection from temperature elevation according to above parameters is suggested.

Animals↗

Importance of structural features for tRNA(Met) identity.

We showed previously that the tRNA tertiary structure makes an important contribution to the identity of yeast tRNA(Met) (Senger B, Aphasizhev R, Walter P, Fasiolo F, 1995, J Mol Biol 249:45-58). To learn more about the role played by the tRNA framework, we analyzed the effect of some phosphodiester cleavages and 2'OH groups in tRNA binding and aminoacylation. The tRNA is inactivated provided the break occurs in the central core region responsible for the tertiary fold or in the anticodon stem/loop region. We also show that, for tRNA(Met) to bind, the anticodon loop, but not the anticodon stem, requires a ribosephosphate backbone. A tertiary mutant of yeast tRNA(Met) involving interactions from the D- and T-loop unique to the initiator species fails to be aminoacylated, but still binds to yeast methionyl-tRNA synthetase. In the presence of 10 mM MgCl2, the mutant transcript has a 3D fold significantly stabilized by about 30 degrees C over a wild-type transcript as deduced from the measure of their T(m) values. The k(cat) defect of the tRNA(Met) mutant may arise from a failure to overcome an increase of the free energetic cost of distorting the more stable tRNA structure and/or a tRNA based MetRS conformational change required for formation of transition state of aminoacylation.

Anticodon↗

Red blood cell adhesion on a solid/liquid interface.

Red blood cells (RBCs), previously fixed with glutaraldehyde, adhere to glass slides coated with fibrinogen. The RBC deposition process on the horizontal glass surface is investigated by analyzing the relative surface covered by the RBCs, as well as the variance of this surface coverage, as a function of the concentration of particles. This study is performed by optical microscopy and image analysis. A model, derived from the classical random sequential adsorption model, has been developed to account for the experimental results. This model highlights the strong influence of the hydrodynamic interactions during the deposition process.

Adsorption↗

Conservation in evolution for a small monomeric phenylalanyl-tRNA synthetase of the tRNA(Phe) recognition nucleotides and initial aminoacylation site.

We previously showed that yeast mitochondrial phenylalanyl-tRNA synthetase (MSF protein) is evolutionarily distant to the cytoplasmic counterpart based on a high degree of divergence in protein sequence, molecular mass, and quaternary structure. Using yeast cytoplasmic tRNA(Phe) which is efficiently aminoacylated by MSF protein, we report here the tRNA(Phe) primary site of aminoacylation and the identity determinants for MSF protein. As for the cytoplasmic phenylalanyl-tRNA synthetase (Sampson, J. R., Di Renzo, A. B., Behlen, L. S., & Uhlenbeck, O. C. (1989) Science 243, 1363-1366), MSF protein recognizes nucleotides from the anticodon and the acceptor end including base A73 and, as shown here, adjacent G1-C72 base pair or at least C72 base. This indicates that the way of tRNA(Phe) binding for the two phenylalanine enzymes is conserved in evolution. However, tRNA(Phe) tertiary structure seems more critical for the interaction with the cytoplasmic enzyme than with MSF protein, and unlike cytoplasmic phenylalanyl-tRNA synthetase, the small size of the monomeric MSF protein probably does not allow contacts with residue 20 at the top corner of the L molecule. We also show that MSF protein preferentially aminoacylates the terminal 2'-OH group of tRNA(Phe) but with a catalytic efficiency for tRNA(Phe)-CC-3'-deoxyadenosine reduced 100-fold from that of native tRNA(Phe), suggesting a role of the terminal 3'-OH in catalysis. The loss is only 1.5-fold when tRNA(Phe)-CC-3'-deoxyadenosine is aminoacylated by yeast cytoplasmic PheRS (Sprinzl, M., & Cramer, F. (1973) Nature 245, 3-5), indicating mechanistic differences between the two PheRS's active sites for the amino acid transfer step.

Amino Acid Sequence↗

Yeast tRNA(Met) recognition by methionyl-tRNA synthetase requires determinants from the primary, secondary and tertiary structure: a review.

The primordial role of the CAU anticodon in methionine identity of the tRNA has been established by others nearly a decade ago in Escherichia coli and yeast tRNA(Met). We show here that the CAU triplet alone is unable to confer methionine acceptance to a tRNA. This requires the contribution of the discriminatory base A73 and the non-anticodon bases of the anticodon loop. To better understand the functional communication between the anticodon and the active site, we analysed the binding and aminoacylation of tRNA(Met) based anticodon and acceptor-stem minihelices and of tRNA(Met) chimeras where the central core region of yeast tRNA(Met) is replaced by that of unusual mitochondrial forms lacking either a D-stem or a T-stem. These studies suggest that the high selectivity of the anticodon bases in tRNA(Met) implies the L-conformation of the tRNA and the presence of a D-stem. The importance of a L-structure for recognition of tRNA(Met) was also deduced from mutations of tertiary interactions known to play a general role in tRNA(Met) folding.

Amino Acid Sequence↗

The presence of a D-stem but not a T-stem is essential for triggering aminoacylation upon anticodon binding in yeast methionine tRNA.

Dissection of the yeast cytoplasmic initiator tRNA(Met) into two helical domains, the T psi C acceptor and anticodon minihelices, failed to show anminoacylation and binding of the acceptor minihelix by the yeast methionyl-tRNA synthetase (MetRS) even in the presence of the anticodon minihelix. In contrast, based on the measure of the inhibition constant Ki, the anticodon minihelix carrying the methionine anticodon CAU is specifically bound to the synthetase and with an affinity comparable to that of the full-length tRNA. The yeast tRNA(Met) acceptor and anticodon minihelices were covalently linked using the central core sequences of either bovine mitochondrial tRNA(Ser) (AGY) lacking a D-stem or initiator tRNA(Met) from Caenorhabditis elegans lacking a T-stem. Based on modeling studies of analogous constructs performed by others, we assume that the folding and distance between the anticodon and acceptor ends of these hybrid tRNAs are identical to that of canonical tRNA. The three-quarter molecule, which includes the T-stem, has aminoacylation activity significantly more than an acceptor minihelix, while the acceptor stem/anticodon-D stem biloop has near wild-type aminoacylation activity. These results suggest that the high selectivity of the anticodon bases in tRNA(Met) depends upon the tRNA L-shape conformation and the presence of a D-arm. Protein contacts with the D-arm phosphate backbone are required for connecting anticodon recognition with the active site. These interactions probably contribute to fine tune the position of the acceptor end in the active site, allowing entry into the transition state of aminoacylation upon anticodon binding. The importance of an L structure for recognition of tRNA(Met) by yeast MetRS was also deduced from mutations of tertiary interactions known to play a general role in tRNA folding.

Acylation↗

[Rheologic and biophysical aspects of cellular adhesion and aggregation: importance in hemorheology].

Interactions between blood cells in the form of cellular aggregates or adhesion are observed in a variety of normal and pathological conditions. Aggregation of erythrocytes or platelets, adhesion of platelets and leucocytes and immune agglutination of RBC are examples of interactions involving blood cells. Cell adhesion and aggregation are modulated by specific interactions (antigen-antibodies reactions, adhesive macromolecules interactions...) or non-specific (van der Waals forces, electrostatic interactions, molecular bridgings...). These interactions may result in morphological and structural changes, or polarization phenomena. At the dynamic level, cellular adhesion (or aggregation) can divided in 4 main steps: transport, cellular activation (endogenous or exogenous), morphological, physical or steric rearrangements, contact (intercellular or on an artificial surfaces). It will be the nature of the interactions involved in these steps that will determine the binding cohesion and kinetic. In this paper, different types of interactions and the regulation mechanisms of adhesion and aggregation phenomena involved in blood hemodynamics will be summarized and some examples (RBC or platelets aggregation; platelets or leucocytes adhesion) will illustrate the importance of these phenomena in clinical hemorheology.

Biophysical Phenomena↗

Fluctuation of the number of particles deposited on a flat surface by a random sequential adsorption mechanism.

The problem of the fluctuations of the number n of particles adsorbed on surfaces through a random sequential adsorption process is discussed. Attention is paid, in particular, to the effect of the size of the adsorbing surfaces upon the variance sigma2(n) of this number. On the basis of computer simulations, it is shown that sigma2(n) is not proportional to the area a of the surface but can be written as a sum of three contributions, which are proportional to a, a1/2, and a0. A theoretical estimate based on the relation between the radial distribution function g(r) and the fluctuation is presented and provides a basis for these findings. This analysis is of general validity and can, in particular, also be applied to the equilibrium case (in the absence of a phase transition) and to the ballistic deposition process.

Journal Article↗

Intron-dependent formation of pseudouridines in the anticodon of Saccharomyces cerevisiae minor tRNA(Ile).

We have isolated and sequenced the minor species of tRNA(Ile) from Saccharomyces cerevisiae. This tRNA contains two unusual pseudouridines (psi s) in the first and third positions of the anticodon. As shown earlier by others, this tRNA derives from two genes having an identical 60 nt intron. We used in vitro procedures to study the structural requirements for the conversion of the anticodon uridines to psi 34 and psi 36. We show here that psi 34/psi 36 modifications require the presence of the pre-tRNA(Ile) intron but are not dependent upon the particular base at any single position of the anticodon. The conversion of U34 to psi 34 occurs independently from psi 36 synthesis and vice versa. However, psi 34 is not formed when the middle and the third anticodon bases of pre-tRNA(Ile) are both substituted to yield ochre anticodon UUA. This ochre pre-tRNA(Ile) mutant has the central anticodon uridine modified to psi 35 as is the case for S.cerevisiae SUP6 tyrosine-inserting ochre suppressor tRNA. In contrast, neither the first nor the third anticodon pseudouridine is formed, when the ochre (UUA) anticodon in the pre-tRNA(Tyr) is substituted with the isoleucine UAU anticodon. A synthetic mini-substrate consisting of the anticodon stem and loop and the wild-type intron of pre-tRNA(Ile) is sufficient to fully modify the anticodon U34 and U36 into psi s. This is the first example of the tRNA intron sequence, rather than the whole tRNA or pre-tRNA domain, being the main determinant of nucleoside modification.

Anticodon↗

Modulation of the suppression efficiency and amino acid identity of an artificial yeast amber isoleucine transfer RNA in Escherichia coli by a G-U pair in the anticodon stem.

The artificial amber suppressor corresponding to the major isoleucine tRNA from yeast (pVBt5), when expressed in E. coli, is a poor suppressor of the amber mutation lacIam181-Z. By analysing mutant forms, we could show that this was due to the presence of a U30-G40 wobble pair in the anticodon stem of the yeast tRNA and not to the level of the heterologously expressed tRNA. Efficient suppressors were obtained by restoring a normal U30-A40 or G30-C40 Watson-Crick pair. In vivo the mutant forms are exclusively charged by the bacterial lysyl-tRNA synthetase (LysRS), whereas the original yeast amber tRNA is charged at a low level by E. coli glutaminyl-tRNA synthetase (GlnRS) and LysRS. The inversion of the U30-G40 pair also induces a loss of the Gln identity. We conclude from these experiments that the U30-G40 base pair constitutes a negative determinant for LysRS interaction which operates either at the level of complex formation or at the catalytic step. As no direct contacts are seen between GlnRS and positions 30-40 of the complexed homologous tRNA, the U30-G40 pair of pVBt5 is believed to influence aminoacylation by GlnRS indirectly, probably at the level of the anticodon loop conformation by favouring an optimal apposition of the anticodon nucleotides with the protein.

Amino Acyl-tRNA Synthetases↗

Adhesion of hard spheres under the influence of double-layer, van der Waals, and gravitational potentials at a solid/liquid interface.

The deposition process of colloidal particles or microorganisms on flat surfaces is analyzed by means of computer simulations. Interparticle interactions (double layer and van der Waals) and weak gravitational forces are taken into account; hydrodynamic interactions, on the other hand, are neglected. In particular, the deposition probability as a function of the deposition location of a particle in the presence of one or two identical fixed particles is discussed. It is shown, in particular, that the ratio of the adhesion probabilities at a given location r, for particles subject to weak gravitation, in the presence and in the absence of the interparticle interaction U(r) follows approximately a Boltzmann law exp[-U(r)/kT], even though the adsorption process is fully irreversible. This result validates, as far as the distribution function of particles on a surface is concerned, Adamczyk's assumption [Adamczyk, Z., Zembala, M., Siwek, B. & Warszynski, P. (1990) J. Colloid Interface Sci. 140, 123-137] that the adhesion process of Brownian particles can be modeled by a random sequential adsorption model with an adsorption probability equal to exp[-U(r)/kT].

Adsorption↗

Influence of diffusion and gravity on the adhesion of a two-component mixture of hard spheres on a flat surface.

The adhesion of hard spheres, modeling particles of biological interest (proteins, bacteria, cells), on flat surfaces is investigated by means of Monte Carlo simulations. These computations include the Brownian diffusion of the particles in the bulk fluid, as well as the systematic displacement due to the gravitational field. The size of the particles influences directly both diffusion coefficient and net weight, with the consequence that the coverage at the jamming limit depends on this parameter. Results obtained in a former paper based on a lattice model are confirmed by the present continuous space model. In order to gain a better understanding of the adsorption competition of two types of particles, the proposed model is applied to the case of binary mixtures of spheres. For polydispersed suspensions, various parameters determine the final coverage, as well as the distribution of the small and large particles on the surface: the radii of the particles and the respective proportions of them in the infinitely large reservoir from which they are randomly selected. In this way, it is shown that the chronology of the adhesion of the small and large particles strongly influences the final number of each type of spheres fixed on the surface. Qualitatively, the present results resemble those obtained with disks placed by means of a classical random sequential adsorption mechanisms. Quantitatively, however, the number densities and coverage values determined in this way are significantly different due to the inclusion of the gravity and of the diffusion in the model.

Adhesiveness↗