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A general-purpose method is presented and implemented to express analytically one stationary configuration of an ideal 3D elastic rod when the end-to-end relative position and orientation are imposed. The mechanical equilibrium of such a rod is described by ordinary differential equations and parametrized by six scalar quantities. When one end of the rod is anchored, the analytical integration of these equations lead to one unique solution for given values of these six parameters. When the second end is also anchored, six additional nonlinear equations must be resolved to obtain parameter values that fit the targeted boundary conditions. We find one solution of these equations with a zero-finding algorithm, by taking initial guesses from a grid of potential candidates. We exhibit the symmetries of the problem, which reduces drastically the size of this grid and shortens the time of selection of an initial guess. The six variables used in the search algorithm, forces and moments at one end of the rod, are particularly adapted due to their unbounded definition domain. More than 850 000 tests are performed in a large region of configurational space, and in 99.9% of cases the targeted boundary conditions are reached with short computation time and a precision better than 10 − 5 . We propose extensions of the method to obtain many solutions instead of only one, using numerical continuation or starting from different initial guesses.

The GGQ minidomain of the ribosomal protein eL42 was previously shown to contact the CCA-arm of P-site bound tRNA in human ribosome, indicating a possible involvement of the protein in the catalytic activity. Here, using Schizosaccharomyces pombe (S. pombe) cells, we demonstrate that the GGQ minidomain and neighboring region of eL42 is critical for the ribosomal function. Mutant eL42 proteins containing amino acid substitutions within or adjacent to the GGQ minidomain failed to complement the function of wild-type eL42, and expression of the mutant eL42 proteins led to severe growth defects. These results suggest that the mutations in eL42 interfere with the ribosomal function in vivo. Furthermore, we show that some of the mutations associated with the conserved GGQ region lead to reduced activities in the poly(Phe) synthesis and/or in the peptidyl transferase reaction with respect to puromycin, as compared with those of the wild-type ribosomes. A pK value of 6.95 was measured for the side chain of Lys-55/Arg-55, which is considerably less than that of a Lys or Arg residue. Altogether, our findings suggest that eL42 contributes to the 80S ribosome's peptidyl transferase activity by promoting the course of the elongation cycle.

International audience; In this report, we have used periodate-oxidized tRNA (tRNAox) as an affinity laleling reagent to demonstrate that: (i) the bL12 protein contacts the CCA-arm of Psite bound tRNA on the Escherichia coli 70S ribosomes; (ii) the stoichiometry of labelling is one molecule of tRNAox bound to one polypeptide chain of endogenous bL12; (iii) cross-linking in situ of bL12 with tRNAox on the ribosomes provokes the loss of activity; (iv) intact tRNA protects bL12 in the 70S ribosomes against cross-linking with tRNAox; (v) both tRNAox and pyridoxal 50-phosphate (PLP) compete for the same or for proximal cross-linking site(s) on bL12 inside the ribosome; (vi) the stoichiometry of cross-linking of PLP to the recombinant E. coli bL12 protein is one molecule of PLP covalently bound per polypeptide chain; (vii) the amino acid residue of recombinant bL12 cross-linked with PLP is Lys-65; (viii) Lys-65 of E. coli bL12 corresponds to Lys-53 of eL42 which was previously shown to cross-link with P-site bound tRNAox on human 80S ribosomes in situ; (ix) finally, E. coli bL12 and human eL42 proteins display significant primary structure similarities, which argues for evolutionary conservation of these two proteins located at the tRNA-CCA binding site on eubacterial and eukaryal ribosomes.

International audience; We investigate the equilibrium configurations of the ideal 3D elastica, i.e., inextensible, unshearable, isotropic, uniform, and naturally straight and prismatic rods, with linear elastic constitutive relations. Infinite solution trajectories are expressed analytically and classified in terms of only three parameters related to physical quantities. Orientation of sections and mechanical loading are also well described analytically with these parameters. Detailed analysis of solution trajectories yields two main results. First, all particular trajectories are completely characterized and located in the space of these parameters. Second, a general geometric structure is exhibited for every ideal 3D elastic rod, where the trajectory winds around a core helix in a tube-shaped envelope. This remarkable structure leads to a classification of the general case according to three properties called chirality components. In addition, the geometry of the envelope provides another characterization of the ideal 3D elastica. For both results, the domains and the frontiers of every class are plotted in the space of the parameters

Mucin 1 is a well-established target for the early diagnosis of epithelial cancers. The nucleotides of the S1.3/S2.2 DNA aptamer involved in binding to variable number tandem repeat mucin 1 peptides have been identified using footprinting experiments. The majority of these binding nucleotides are located in the 25-nucleotide variable region of the total aptamer. Imino proton and 2D NMR spectra of truncated and total aptamers in supercooled water reveal common hydrogen-bonding networks and point to a similar secondary structure for this 25-mer sequence alone or embedded within the total aptamer. NMR titration experiments confirm that the TTT triloop structure is the primary binding site and show that the initial structure of the truncated aptamers is conserved upon interaction with variable number tandem repeat peptides. The thermal dependence of the NMR chemical shift data shows that the base-paired nucleotides melt cooperatively at 47 ± 4°C. The structure of the 25-mer oligonucleotide was determined using a new combined mesoscale molecular modeling, molecular dynamics and NMR spectroscopy investigation. It contains three Watson-Crick pairs, three consecutive mispairs and four Watson-Crick pairs capped by a TTT triloop motif. The 3D model structures (PDB 2L5K) and biopolymer chain elasticity molecular models are consistent with both NMR and long unconstrained molecular dynamics (10 ns) in explicit water, respectively. Database Structural data are available in the Protein Data Bank and BioMagResBank databases under the accession numbers 2L5K and 17129, respectively.

Determination of DNA solution structure is a difficult task even with the high-sensitivity method used here based on simulated annealing with 35 restraints/residue (Cryoprobe 750 MHz NMR). The conformations of both the phosphodiester linkages and the dinucleotide segment encompassing the sharp turn in single-stranded DNA are often underdetermined. To obtain higher quality structures of a DNA GNRA loop, 5'-d(GCGAAAGC)-3', we have used a mesoscopic molecular modeling approach, called Biopolymer Chain Elasticity (BCE), to provide reference conformations. By construction, these models are the least deformed hairpin loop conformation derived from canonical B-DNA at the nucleotide level. We have further explored this molecular conformation at the torsion angle level with AMBER molecular mechanics using different possible (epsilon,zeta) constraints to interpret the 31P NMR data. This combined approach yields a more accurate molecular conformation, compatible with all the NMR data, than each method taken separately, NMR/DYANA or BCE/AMBER. In agreement with the principle of minimal deformation of the backbone, the hairpin motif is stabilized by maximal base-stacking interactions on both the 5'- and 3'-sides and by a sheared G.A mismatch base pair between the first and last loop nucleotides. The sharp turn is located between the third and fourth loop nucleotides, and only two torsion angles beta6 and gamma6 deviate strongly with respect to canonical B-DNA structure. Two other torsion angle pairs epsilon3,zeta3 and epsilon5,zeta5 exhibit the newly recognized stable conformation BIIzeta+ (-70 degrees, 140 degrees). This combined approach has proven to be useful for the interpretation of an unusual 31P chemical shift in the 5'-d(GCGAAAGC)-3' hairpin.

Successive investigations over the last decade have revealed and confirmed a stable loop closure in a family of d-[GTAC-5Pur6N7N-GTAC] hairpins, where 5Pur6N7N is a AAA, GAG and AXC loop (X being any nucleotide). The trinucleotide loop is characterized by a well defined 5Pur-7N mispairing mode, and by upfield chemical shifts for three sugar protons of the apical nucleotide 6N. The GTTC-ACA-GAAC DNA hairpin, of interest for its likely involvement in Vibrio cholerae genome mutations, has now been investigated. The GTAC-ACA-GTAC DNA hairpin has also been studied because it is intermediate between the other structures, as it contains the loop of the hairpin under consideration and the stem of the above family. The two hairpins with the ACA loop are stable. They show the same mispairing mode and similar upfield shifts as the previous family, but GTTC-ACA-GAAC seems to be slightly less compact than any other. GTTC-ACA-GAAC is remarkable in that it exhibits a B(II) character for the phosphate-ester conformation at 8Gp9A, together with a swing of the upper hairpin into the major groove that, in particular, brings 6CH1' roughly as close to 7AH2 as to 6CH6. These unexpected structural features are qualitatively deduced from (1)H and (31)P NMR spectra, and confirmed by Raman spectroscopy. This comparative study shows that not only the loop sequence but also the stem sequence may control hairpin structures.

The "RNA world" hypothesis proposes that early in the evolution of life, RNA was responsible both for the storage and transfer of genetic information and for the catalysis of biochemical reactions. One of the problems of the hypothesis is that RNA is known to be temperature sensitive. Nevertheless, different types of sequences with a thermostable phenotype may exist. In order to test this possibility, we applied an in vitro evolution method (SELEX) to isolate RNA molecules that are resistant at high temperatures (80 degrees C for 65 h) and high salt concentrations (2 M NaCl). The sequences of the resulting cloned halo-thermophilic RNAs can be grouped in two families (I and II) possessing very different thermal and chemical stabilities and very different secondary structures. The selected RNA molecules illustrate two different possibilities leading to thermal resistance which may be related to primitive conditions. We propose that members of family I constitute a good means of storing sequence information while members of family II are less efficient but replicate faster in early steps of the SELEX. These selected RNA behaviors may be related to primitive conditions and could allow to define limits for survival, and demonstrate that what is at stake for RNA molecules, as for living organisms, is survival and reproduction.

The presence of a N-(2-deoxy-D-erythro pentofuranosyl)urea (henceforth referred to as deoxyribosylurea) residue, ring fragmentation product of a thymine, in a frameshift situation in the sequence 5'd(AGGACCACG).d(CGTGGurTCCT) has been studied by 1H and 31P nuclear magnetic resonance and molecular dynamics. At equilibrium, two species are found in slow exchange. We observe that the deoxyribosylurea residue can be either intra- or extrahelical within structures which otherwise do not deviate strongly from that of a B-DNA as observed by NMR. Our study suggests that this is determined by the nature and number of hydrogen bonds which this residue can form as a function of two possible isomers. There are two possible structures for the urea side chain, either cis or trans for the urido bond which significantly changes the hydrogen bonding geometry of the residue. In the intrahelical species, the cis isomer can form two good hydrogen bonds with the bases on the opposite strand in the intrahelical species, A4 and C5, which is not the case for the trans isomer. This results in a kink in the helical axis. For the major extrahelical species, the situation is reversed. The trans isomer is able to form two good hydrogen bonds, with G13 on the same strand and A7 on the opposite strand. For the extrahelical species, the cis isomer can form only one hydrogen bond. In this major structure the NMR data show that the bases which are on either side of the deoxyribosylurea residue in the sequence, G14 and T16, are stacked over each other in a way similar to a normal B-DNA structure. This requires the formation of a loop for the backbone between these two residues. This loop can belong to one of two families, right- or left-handed. In a previous study of an abasic frameshift [Cuniasse et al. (1989) Biochemistry 28, 2018-2026], a left-handed loop was observed, whereas in this study a right-handed loop is found for the first time in solution. The deoxyribosylurea residue lies in the minor groove and can form both an intra- and an interstrand hydrogen bond.

Two mismatches, G.G and I.I, have been incorporated at the central position of 5'd-(GCCACXAGCTC).d(GAGCTXGTGGC) in order to carry out NMR and molecular dynamics studies. These duplexes constitute the sequence 29-39 of the K-ras gene coding for the glycine 12, a hot spot for mutation. The NMR spectra show that the duplexes are not greatly distorted by the introduction of the mismatches and their global conformation is that of a canonical B-form double helix. For the duplex containing the G.G mismatch, we propose for the major species, a type of pairing involving one hydrogen bond between the imino group of one central guanine and the carbonyl group of the opposite guanine. Both bases are in an anti conformation. Two conformations, with the same donor and acceptor pattern can coexist, one is obtained from the other by a 180 degrees rotation about the pseudodyadic axis. Exchange between the two forms is observed by NMR at low temperature. A minor species involving hydrogen bonding between the guanine amino group and the carbonyl group of the guanine on the opposite strand may also exist as shown by the molecular dynamics calculations. For the I.I mismatch we observe the same major species, i.e., hydrogen bonding between an imino proton of one base and the carbonyl group of the base on the opposite strand with both bases in an anti conformation. Exchange between these two conformations is faster than for the G.G mismatch. Further, we observe that the I.I mismatch adopts a minor conformation, in which one or other of the bases is in the syn conformation.

Background The Signal Transducer and Activator of Transcription 3 (STAT3) is activated in tumor cells, and STAT3-inhibitors are able to induce the death of those cells. Decoy oligodeoxynucleotides (dODNs), which bind to the DNA Binding Domain (DBD) of STAT3, are efficient inhibitors. However, they also inhibit STAT1, whose activity is essential not only to resistance to pathogens, but also to cell growth inhibition and programmed cell death processes. The aim of this study was to design STAT3-specific dODNs which do not affect STAT1-mediated processes. Results New dODNs with a hairpin (hpdODNs) were designed. Modifications were introduced, based on the comparison of STAT3- and STAT1-DBD interactions with DNA using 3D structural analyses. The designed hpdODNs were tested for their ability to inhibit STAT3 but not STAT1 by determining: i) cell death in the active STAT3-dependent SW480 colon carcinoma cell line, ii) absence of inhibition of interferon (IFN) γ-dependent cell death, iii) expression of STAT1 targets, and iv) nuclear location of STAT3 and STAT1. One hpdODN was found to efficiently induce the death of SW480 cells without interfering with IFNγ-activated STAT1. This hpdODN was found in a complex with STAT3 but not with STAT1 using an original in-cell pull-down assay; this hpdODN also did not inhibit IFNγ-induced STAT1 phosphorylation, nor did it inhibit the expression of the STAT1-target IRF1. Furthermore, it prevented the nuclear transfer of STAT3 but not that of IFNγ-activated STAT1. Conclusions Comparative analyses at the atomic level revealed slight differences in STAT3 and STAT1 DBDs' interaction with their DNA target. These were sufficient to design a new discriminating hpdODN that inhibits STAT3 and not STAT1, thereby inducing tumor cell death without interfering with STAT1-dependent processes. Preferential interaction with STAT3 depends on oligodeoxynucleotide sequence modifications but might also result from DNA shape changes, known to modulate protein/DNA interactions. The finding of a STAT3-specific hpdODN establishes the first rational basis for designing STAT3 DBD-specific inhibitors.

Mucin 1 is a well-established target for the early diagnosis of epithelial cancers. The nucleotides of the S1.3/S2.2 DNA aptamer involved in binding to variable number tandem repeat mucin 1 peptides have been identified using footprinting experiments. The majority of these binding nucleotides are located in the 25-nucleotide variable region of the total aptamer. Imino proton and 2D NMR spectra of truncated and total aptamers in supercooled water reveal common hydrogen-bonding networks and point to a similar secondary structure for this 25-mer sequence alone or embedded within the total aptamer. NMR titration experiments confirm that the TTT triloop structure is the primary binding site and show that the initial structure of the truncated aptamers is conserved upon interaction with variable number tandem repeat peptides. The thermal dependence of the NMR chemical shift data shows that the base-paired nucleotides melt cooperatively at 47 ± 4°C. The structure of the 25-mer oligonucleotide was determined using a new combined mesoscale molecular modeling, molecular dynamics and NMR spectroscopy investigation. It contains three Watson-Crick pairs, three consecutive mispairs and four Watson-Crick pairs capped by a TTT triloop motif. The 3D model structures (PDB 2L5K) and biopolymer chain elasticity molecular models are consistent with both NMR and long unconstrained molecular dynamics (10 ns) in explicit water, respectively. Database Structural data are available in the Protein Data Bank and BioMagResBank databases under the accession numbers 2L5K and 17129, respectively.

International audience; UV irradiation at 254 nm of 2'-O,5-dimethyluridylyl(3'-5')-2'-O,5-dimethyluridine (1a) and of natural thymidylyl(3'-5')thymidine (1b) generates the same photoproducts (CPD and (6-4)PP; responsible for cell death and skin cancer). The ratios of quantum yields of photoproducts obtained from 1a (determined herein) to that from 1b are in a proportion close to the approximately threefold increase of stacked dinucleotides for 1a compared with those of 1b (from previous circular dichroism results). 1a and 1b however are endowed with different predominant sugar conformations, C3'-endo (1a) and C2'-endo (1b). The present investigation of the stacked conformation of these molecules, by unrestrained state-of-the-art molecular simulation in explicit solvent and salt, resolves this apparent paradox and suggests the following main conclusions. Stacked dinucleotides 1a and 1b adopt the main characteristic features of a single-stranded A and B form, respectively, where the relative positions of the backbone and the bases are very different. Unexpectedly, the geometry of the stacking of two thymine bases, within each dinucleotide, is very similar and is in excellent agreement with photochemical and circular dichroism results. Analyses of molecular dynamics trajectories with conformational adiabatic mapping show that 1a and 1b explore two different regions of conformational space and possess very different flexibilities. Therefore, even though their base stacking is very similar, these molecules possess different geometrical, mechanical, and dynamical properties that may account for the discrepancy observed between increased stacking and increased photoproduct formations. The computed average stacked conformations of 1a and 1b are well-defined and could serve as starting models to investigate photochemical reactions with quantum dynamics simulations.

A new molecular modelling methodology is presented and shown to apply to all published solution structures of DNA hairpins with TTT in the loop. It is based on the theory of elasticity of thin rods and on the assumption that single-stranded B-DNA behaves as a continuous, unshearable, unstretchable and flexible thin rod. It requires four construction steps: (i) computation of the tri-dimensional trajectory of the elastic line, (ii) global deformation of single-stranded helical DNA onto the elastic line, (iii) optimisation of the nucleoside rotations about the elastic line, (iv) energy minimisation to restore backbone bond lengths and bond angles. This theoretical approach called 'Biopolymer Chain Elasticity' (BCE) is capable of reproducing the tri-dimensional course of the sugar-phosphate chain and, using NMR-derived distances, of reproducing models close to published solution structures. This is shown by computing three different types of distance criteria. The natural description provided by the elastic line and by the new parameter, Omega, which corresponds to the rotation angles of nucleosides about the elastic line, offers a considerable simplification of molecular modelling of hairpin loops. They can be varied independently from each other, since the global shape of the hairpin loop is preserved in all cases.

The biopolymer chain elasticity (BCE) approach and the new molecular modelling methodology presented previously are used to predict the tri- dimensional backbones of DNA and RNA hairpin loops. The structures of eight remarkably stable DNA or RNA hairpin molecules closed by a mispair, recently determined in solution by NMR and deposited in the PDB, are shown to verify the predicted trajectories by an analysis automated for large numbers of PDB conformations. They encompass: one DNA tetraloop, -GTTA-; three DNA triloops, -AAA- or -GCA-; and four RNA tetraloops, -UUCG-. Folding generates no distortions and bond lengths and bond angles of main atoms of the sugar-phosphate backbone are well restored upon energy refinement. Three different methods (superpositions, distance of main chain atoms to the elastic line and RMSd) are used to show a very good agreement between the trajectories of sugar-phosphate backbones and between entire molecules of theoretical models and of PDB conformations. The geometry of end conditions imposed by the stem is sufficient to dictate the different characteristic DNA or RNA folding shapes. The reduced angular space, consisting of the new parameter, angle Omega, together with the chi angle offers a simple, coherent and quantitative description of hairpin loops.

The conformational changes induced by the binding of the histone-like protein MC1 to DNA duplexes have been analyzed by dark-field electron microscopy and polyacrylamide gel electrophoresis. Visualisation of the DNA molecules by electron microscopy reveals that the binding of MC1 induces sharp kinks. Linear DNA duplexes (176 bp) which contained a preferential site located at the center were used for quantitative analysis. Measurements of the angle at the center of all duplexes, at a fixed DNA concentration, as a function of the MC1 concentration, were very well fitted by a simple model of an isotropic flexible junction and an equilibrium between the two conformations of DNA with bound or unbound MC1. This model amounts to double-folded Gaussian distributions and yields an equilibrium deflection angle of θ 0 =116 ° for the DNA with bound MC1. It allowed measurements of the fraction of DNA with bound MC1 to be taken as a function of MC1 concentrations and yields an equilibrium dissociation constant of K d =100 nM. It shows that the flexibility of DNA is reduced by the binding of MC1 and the formation of a kink. The equilibrium dissociation constant value was corroborated by gel electrophoresis. Control of the model by the computation of the reduced χ 2 shows that the measurements are consistent and that electron microscopy can be used to quantify precisely the DNA deformations induced by the binding of a protein to a preferential site.

The conformational changes induced by the introduction of a central and unique single-stranded break in a 139 base-pair DNA duplex have been analysed by means of polyacrylamide gel electrophoresis, HPLC and dark-field electron microscopy. Compared to the control DNA, the disruption of the covalent sugar-phosphate backbone induces a retardation detected both by gel electrophoresis and anion exchange based HPLC. Electron microscopic visualization of the DNA molecules reveals that most of them present a central fracture at the position of the nick. Measures of the angle at the apex were very well fitted by a simple model of isotropic flexible junction assuming spatial Hooke's law and simple basic Boltzmann statistics. This amounts to using a folded Gaussian distribution. The fit yields an angle equilibrium value phi 0 = 122 degrees for the nicked fragment. The angle distribution could also result from an equilibrium between two forms of the molecule with isotropic flexibility at the nicked site: a stacked and a very flexible unstacked form. The majority of bound poly(ADP-ribose) polymerase, a zinc-finger enzyme involved in DNA break detection, was localized at the apex of the V-shaped DNA duplex, with an accentuation of its general V-shaped conformation (phi 0 = 102 degrees).

The kinetics of the reaction of acetyl coenzyme A (AcCoA) with fatty acid synthase has been studied with a modified quenched-flow technique in 0.1 M potassium phosphate (pH 7.0), 0.5 mM ethylenediaminetetraacetic acid, and 10% glycerol (w/v) at 23 degrees C. The kinetics of the deacetylation of the isolated acetylated enzyme by CoA also was studied. An overall mechanism consistent with the data is (formula; see text) where E represents the enzyme. The equilibrium dissociation constants, K1 and K3, were estimated to be 85 and 70 microM, respectively, and the rate constants k2 and k-2 are 43 and 103 s-1, respectively. The maximum number of acetyl groups bound to the enzyme in terms of this mechanism is 3.8 (mol/mol). This mechanism also is consistent with the amount of acetylated enzyme formed during titrations of the enzyme and radioactive AcCoA with CoA. The spontaneous hydrolysis of the enzyme at 23 degrees C has a rate constant of 4.7 X 10(-4) s-1. The acetyl groups on the native enzyme are rapidly removed by hydroxylamine. However, 0.39 of the acetyl groups remains after treatment with hydroxylamine if the enzyme is first denatured in 4 M urea. This suggests that the acyl binding sites on the native enzyme are an unstable acetyl oxygen ester and an acetyl thio ester. Destruction of the thioesterase activity of the enzyme through chemical modification of the enzyme does not alter the rate of spontaneous hydrolysis of the acetyl-enzyme nor its reactivity toward hydroxylamine.

The following reactions catalyzed by chicken liver fatty acid synthase have been studied with the stopped-flow method in 0.1 M potassium phosphate (pH 7.0) and 1 mM ethylenediaminetetraacetic acid at 25 degrees C by monitoring the change in NADPH fluorescence: the transfer of acetoacetyl from acetoacetyl coenzyme A to the enzyme, reduction of the enzyme-bound acetoacetyl by NADPH (beta-ketoacyl reductase), and reduction of enzyme-bound D-hydroxybutyryl/crotonyl by NADPH (enoyl reductase). The first two reactions were studied by mixing enzyme-NADPH with acetoacetyl-CoA under conditions where the kinetics can be analyzed as two consecutive pseudo-first-order processes: a mechanism consistent with the aceto-acetyl-CoA dependence of the pseudo-first-order rate constant associated with formation of the aceto-acetyl-enzyme is a relatively rapid binding of substrate to the enzyme, with a dissociation constant of 650 microM, followed by formation of covalently bound acetoacetyl, with a rate constant of 10.2 s-1. The aceto-acetyl-enzyme is reduced by enzyme-bound NADPH with a rate constant of 20 s-1, and the NADPH binding is characterized by a dissociation constant of 5.3 microM. Reduction of the D-hydroxybutyryl-/crotonyl-enzyme was studied by mixing NADPH with enzyme that was equilibrated with D-hydroxybutyryl-CoA or crotonyl-CoA; the rate constant for reduction of an equilibrium mixture of D-hydroxybutyryl- and crotonyl-enzyme is 36.6 s-1. Steady-state kinetic studies of the reduction of acetoacetyl-CoA and crotonyl-CoA by NADPH also have been carried out.(ABSTRACT TRUNCATED AT 250 WORDS)

The kinetics of reduced nicotinamide adenine dinucleotide phosphate (NADPH) binding to fatty acid synthase from chicken liver and of the reduction of enzyme-bound acetoacetyl by NADPH (beta-ketoacyl reductase) and the steps leading to formation of the acetoacetyl-enzyme have been studied in 0.1 M potassium phosphate-1 mM ethylenediaminetetraacetic acid (EDTA), pH 7.0, at 25 degrees C by monitoring changes in NADPH fluorescence with a stopped-flow apparatus. Improved fluorescence detection has permitted the use of NADPH concentrations as low as 20 nM. The kinetics of the binding of NADPH to the enzyme is consistent with a simple bimolecular binding mechanism and four equivalent sites on the enzyme (presumably two beta-ketoacyl reductase sites and two enoyl reductase sites). The bimolecular rate constant is 12.7 X 10(6) M-1 s-1, and the dissociation rate constant is 76.7 s-1, which gives an equilibrium dissociation constant of 6.0 microM. The formation of the acetoacetyl-enzyme and its subsequent reduction by NADPH could be analyzed as two consecutive pseudo-first-order reactions by mixing enzyme-NADPH with acetyl-CoA and malonyl-CoA under conditions where [acetyl-CoA], [malonyl-CoA] much greater than [enzyme] much greater than [NADPH]. From the dependence of the rate of reduction of aceto-acetyl-enzyme by NADPH on enzyme concentration, an independent estimate of the equilibrium dissociation constant for NADPH binding to the enzyme of 5.9 microM is obtained, and the rate constant for the reduction is 17.5 s-1.(ABSTRACT TRUNCATED AT 250 WORDS)