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D Porschke

Publications and source records attributed to D Porschke.

At least 37 records · Page 2Linked to original sources
PubMed1990

Permanent dipole moment of tRNA's and variation of their structure in solution.

The structure of six different tRNA molecules has been analyzed in solution by electrooptical measurements and by bead model simulations. The electric dichroism measured as a function of the field strength shows that tRNA's are associated with substantial permanent dipole moments, which are in the range of 1 x 10(-27) cm(identical to 300 D; before correction for the internal directing field). Rotational diffusion time constants of tRNA molecules in their native state at 2 degrees C show a considerable variation. A particularly large value found for tRNA(Tyr) (50 ns) can be explained by its nine additional nucleotide residues. However, remarkable variations remain for tRNA molecules with the standard number of 76 nucleotide residues (tRNA(Phe) [yeast] 41.6 ns, tRNA(Val) [Escherichia coli] 44.9 ns, tRNA(Glu) [E. coli] 46.8 ns; tRNA(Phe) [E. coli] 48.3 ns). These variations indicate modulations of the tertiary structure, which may be due to a change of the L-hinge angle. Bead models are used to simulate both electric and hydrodynamic parameters of tRNA molecules according to the crystal structure of tRNA(Phe) (yeast). The asymmetric distribution of phosphate charges with respect to the center of diffusion leads, under the assumption of a constant charge reduction to 15% by ion condensation, to a theoretical dipole moment of 7.2 x 10(-28) cm, which is in reasonable agreement with the measurements. The dichroism decay curve calculated for tRNA(Phe) (yeast) is also consistent with the measurements and thus the structure in solution and in the crystal must be very similar in this case. However, our measurements also indicate that the structure of some other tRNA's in solution is different, even in cases with the same number of nucleotide residues.

Magnesium↗
PubMed1989

The nature of protein dipole moments: experimental and calculated permanent dipole of alpha-chymotrypsin.

The electric dichroism of alpha-chymotrypsin has been measured in buffers of various pH values and ion compositions. The stationary dichroism obtained as a function of the electric field strength is not compatible with an induced dipole mechanism and clearly shows that alpha-chymotrypsin is associated with a substantial permanent dipole moment. After correction for the internal directing electric field according to a sphere model, the dipole moment is 1.6 X 10(-27) C m at pH 8.3 (corresponding to 480 D). This value decreases with decreasing pH (to 1.2 X 10(-27) C m at pH 4.2), but is almost independent of the monovalent salt concentration in the range from 2 to 12 mM and of Mg2+ addition up to 1 mM. The assignment of the permanent dipole moment is confirmed by analysis of the dichroism rise curves. The dichroism decay time constants of (31 +/- 1) ns at 2 degrees C can be represented by a spherical model with a radius of 25-26 A, which is consistent with the known X-ray structure. The limiting linear dichroism is slightly dependent on the buffer composition and demonstrates subtle variations of the protein structure. As a complement to the experimental results, electric and hydrodynamic parameters of alpha-chymotrypsin have been calculated according to the known X-ray structure. Bead model simulations provide the center of diffusion, which is used to calculate dipole moments according to the equilibrium charge distribution evaluated from standard pK values.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗
PubMed1989

Electric dichroism and bending amplitudes of DNA fragments according to a simple orientation function for weakly bent rods.

The linear dichroism is calculated for DNA fragments in their thermal bending equilibrium. These calculations are given for relatively short fragments, where bent molecules can be described by an arc model. Using the measured value of 350 A for the persistence length, the limit dichroism (corresponding to complete alignment) decreases due to thermal bending, e.g., for a fragment with 100 base pairs to 80% of the value expected for straight molecules. Thermal bending should lead to a strong continuous decrease of the dichroism with increasing chain length, which is not observed, however, in electric dichroism experiments due to electric stretching. The influence of the electric field on the bending equilibrium is described by a contribution to the bending energy, which is calculated from the movement of charge equivalents against the potential gradient upon bending. The charge equivalents, which are assigned to the helix ends, are derived from the dipole moments causing the stationary degree of orientation. By this procedure the energy term inducing DNA stretching is given for induced, permanent, and saturating induced dipole models without introduction of any additional parameter. The stationary dichroism at a given electric field strength is then calculated according to an arc model by integration over all angles of orientation of helix axes or chords with respect to the field vector, and at each of these angles the contribution to the dichroism is calculated by integration over all helices with different degrees of bending. Orientation functions obtained by this procedure are fitted to dichroism data measured for various restriction fragments. Optimal fits are found for an induced dipole model with saturation of the polarizability. The difference between orientation functions with and without electric stretching is used to evaluate dichroism bending amplitudes. Both chain length and field strength dependence of bending amplitudes are consistent with experimental amplitudes derived from the dichroism decay in low salt buffers containing multivalent ions like Mg2+, spermine, or [CoNH3)6]3+. Bending amplitudes can be used to evaluate the persistence length from electrooptical data obtained for a single DNA restriction fragment. Bending and stretching effects are considerable already at relatively low chain length, and thus should not be neglected in any quantitative evaluation of experimental data.

DNA↗
PubMed1989

Effect of aminoacylation on tRNA conformation.

Translational diffusion coefficients have been simulated for various conformations of tRNA(Phe) (yeast) by bead models, in order to analyze data obtained by dynamic light scattering on the free and the aminoacylated form. The 18% increase of the translational diffusion coefficient upon deacylation, reported by Potts et al. (1981), could not be represented by any change of the L-hinge angle, but could only be simulated by a conformation change to an extended form with extensive dissociation of base pairs. Since extensive unpairing is not consistent with evidence accumulated in the literature, the change of the diffusion coefficient must be mainly due to processes other than intramolecular conformational changes.

Acylation↗
PubMed1989

An unusual electrooptical effect observed for DNA fragments and its apparent relation to a permanent electric moment associated with bent DNA.

Dichroism decay curves of DNA fragments with chain lengths in the range of 179-256 bp show an amplitude inversion suggesting the existence of a positive dichroism component, when these fragments are dissolved at monovalent salt concentrations above approx. 5 mM and are exposed to field pulses with amplitudes and/or lengths above critical values. At the critical values, the unusual dichroism is reflected by an apparent acceleration of the decay curves, which can be fitted by single exponentials with time constants much below the values expected from the DNA contour lengths. The critical pulse amplitudes and lengths decrease with increasing DNA chain length and increasing salt concentration. The experimental data are consistent with results obtained by hydrodynamic and electric model calculations on smoothly bent DNA double helices. The DNA is represented by a string of overlapping beads, which is used to calculate the rotational diffusion tensor and the center of diffusion. The distribution of phosphate charges is asymmetric with respect to this center and thus gives rise to a substantial permanent dipole moment. The magnitude of this dipole moment is calculated as a function of DNA curvature and is used together with experimental values of polarizabilities for simulations of dichroism decay curves. The curves simulated for bent DNA show the same phenomenon as observed experimentally. The ionic strength dependence of the unusual dichroism is explained by an independently observed strong decrease of the polarizability with increasing salt concentration. The field strength dependence is probably due to field-induced bending of double helices driven by the change of the dipole moment. Although our calculations are on rigid models of DNA and thus any flexibility of the double helix has not been considered, we conclude that the essential part of our experimental results can be explained by our model.

Circular Dichroism↗
PubMed1988

Structure of the Tet repressor and Tet repressor-operator complexes in solution from electrooptical measurements and hydrodynamic simulations.

The Tet repressor protein and tet operator DNA fragments and their complexes have been analyzed by electrooptical procedures. The protein shows a positive linear dichroism at 280 nm, a negative linear dichroism at 248 nm, and a strong permanent dipole moment of 3.5 X 10(-27) C m, which is independent of the salt concentration within experimental accuracy. Its rotation time constant of 40 ns indicates an elongated structure, which is consistent with a prolate ellipsoid of 100 A for the long axis and 40 A for the short axis. The time constant can also be fitted by a cylinder of length 78 A and diameter 37 A, which is consistent with nuclease protection data reported on repressor-operator complexes, if the cylinder axis is aligned parallel to the DNA axis. Addition of tetracycline induces changes of the limit dichroism but very little change of the rotation time constant. The rotation time constants observed for the operator DNA fragments show some deviations from the values expected from their contour length; however, these deviations remain relatively small. Formation of repressor-operator complexes leads to some increase of the DNA rotation time constants. Simulations by bead models demonstrate that these time constants can be explained without any major change of the hydrodynamic dimension of the components. The data for the complexes are fitted by bead models with smooth bending of the DNA corresponding to a radius of curvature of 500 A, but at the given accuracy, we cannot rule out that the DNA in the complex remains straight or is bent to a smaller radius of approximately 400 A. Thus, binding of the Tet repressor, which is a helix-turn-helix protein as judged from its sequence, to its operator seems to induce minor bending but does not induce strong bending of the DNA double helix.

DNA Transposable Elements↗
PubMed1988

Dynamics of repressor-operator recognition: the Tn10-encoded tetracycline resistance control.

Binding of the Tet repressor to nonspecific and specific DNA leads to quenching of the Tet fluorescence by approximately 22% and approximately 35%, respectively. This effect is used for a direct, quantitative characterization of the binding equilibria and dynamics involved in the recognition of the operator by its repressor. From the dependence of the nonspecific binding constant on the ion concentration, it is concluded that nonspecific binding is almost completely driven by the entropy change resulting from the release of three to four Na+ ions from the double helix upon protein binding. Formation of the specific complex is driven by a higher entropy term resulting from the release of seven to eight Na+ ions and in addition by a free energy term of -33 kJ/mol from nonelectrostatic interactions, which are attributed to the specific contacts. The dynamics of the repressor-operator recognition are resolved by stopped-flow measurements at various salt concentrations and for different DNA chain lengths into two separate steps. The first step follows a second-order mechanism and results in an intermediate complex associated with formation of about three to four electrostatic contacts between protein and DNA; apparently, this complex is equivalent to the nonspecific complex. The existence of an intermediate is also indicated by experiments in mixed Na+-Mg2+ buffers, which can be described with high accuracy by competition of Mg2+ and protein. The intermediate complex is formed at a rate of 3 X 10(8) M-1 s-1 and is converted in the second reaction step to the specific complex with a rate constant of 6 X 10(4) s-1, which is almost independent of the salt concentration. Our interpretation and the parameters obtained from our model are confirmed by competition of nonspecific DNA with operator DNA for repressor binding. The observed maximal rate constant of 3 X 10(8) M-1 s-1 is very close to theoretical predictions for the association without a sliding mechanism. The very small dependence of the observed rate constants on the chain length shows that the Tet repressor is not able to slide over any substantial distance even at low salt concentrations. The question of a potential contribution from sliding under our experimental conditions is critically discussed. The absence of sliding in the case of the Tet repressor under physiological conditions is compared with the high sliding efficiency of the lac repressor and is discussed with respect to possible molecular mechanisms of sliding in relation to biological function.

Base Sequence↗
PubMed1988

Contributions to selective binding of aromatic amino acid residues to tRNA(Phe).

The binding of aromatic amino acid amides to two fragments of tRNA(Phe) has been measured, in order to explore contributions to selective interactions of amino acid residues with tRNA(Phe). Measurements of the Wye base fluorescence demonstrate that the isolated anticodon loop of tRNA(Phe) (15 nucleotide residues) has a binding constant K = 75 M-1 for Phe-amide, which is only slightly lower than that observed previously for the complete tRNA(Phe) (K = 100 M-1). The hexamer GmAAYA psi - possessing most residues of the loop, but without loop structure - shows a further reduced binding constant of 42 M-1. According to these data, part of the selective interaction results from the special loop structure and another part probably from the nature of the Wye base. The particular influence of the loop structure is also demonstrated by binding experiments performed in the presence of Mg2+. As expected, addition of Mg2+ decreases the binding affinity of the aromatic amino acids amides. Moreover, Mg2+ at concentrations greater than or equal to 0.3 mM induces cooperative binding of the amides to the anticodon loop similar to that found previously for the complete tRNA(Phe), whereas the hexamer does not show any indication for cooperativity. A special coupling of Mg2+ and amide binding to the anticodon loop is also indicated by inhibition of Mg2+ binding in the presence of amides, which is much stronger than expected for a simple salt effect. These results demonstrate a complex coupling of Mg2+ and amide binding to different conformational states of the anticodon loop, which resembles an allosteric type of reaction mechanism.

Amides↗
PubMed1988

Turn of promotor DNA by cAMP receptor protein characterized by bead model simulation of rotational diffusion.

The rotation diffusion of DNA double helices and their complexes with the cAMP receptor protein (CRP) has been simulated by bead models, in order to derive information on their structure in solution by comparison with results obtained from dichroism decay measurements. Straight DNA double helices are simulated by linear, rigid strings of overlapping beads. The radius of the beads and the length of the string are increased simultaneously by the same increments from initial outer dimensions derived from crystallographic data to final values, which are fitted to experimental rotation time constants observed for short DNA fragments (less than 100 bp). The final values reflect the solvated structure with the same 'solvation layer' added in all three dimensions. The protein is simulated by overlapping beads, which are assembled to a structure very similar to that found by x-ray crystallography. Complexes of the protein with DNA are formed with the centres of palindromic DNA sites at the centre of the two helix-turn-helix-motifs of the protein with some overlap of the two components. Simulation of the experimental data obtained for CRP complexes with specific DNA in the presence of cAMP requires strong bending of the double helices. According to our simulation the DNA is almost completely wrapped around the protein both in the complexes with a 62 bp fragment containing the standard CRP site and with a 80 bp fragment containing the second binding site of the lac operon. Simulations of the data obtained for a 203 bp fragment with both binding sites suggest that the two bound CRP proteins are in contact with each other and that the DNA is wrapped around the two protein dimers. A stereochemical model is suggested with a tetrahedral arrangement of the four protein subunits, which provides the advantage that two binding sites of the protein formed by two subunits each are located favorable for tight contacts to two binding sites on bent DNA, provided that the DNA sites are separated by an integer number of helix turns. In summary, the simulations demonstrate strong bending, which can be reflected by an arc radius in the range around 50 A. According to these data the overall bending angle of our longest DNA fragment is approximately 180 degrees, and thus the protruding ends are sufficiently close to each other such that RNA polymerase, for example, could contact both helical segments.

DNA↗
PubMed1986

Codon-induced association of the isolated anticodon loop of tRNAPhe.

The binding of the codon UUC to the isolated anticodon loop of tRNAPhe (yeast) has been studied as a model of codon recognition by a simple adaptor. Fluorescence titrations demonstrate that UUC binds to the isolated anticodon loop with an equilibrium constant of 1.4 X 10(3) M-1 (at 7.2 degrees C). Equilibrium sedimentation curves reveal that UUC binding induces association of anticodon loops beyond the dimer stage. A set of complete sedimentation curves obtained for various reactant concentrations was analyzed according to a model with an infinite number of subsequent association steps for UUC-anticodon loop complexes and with equal affinity for each step. The coupling of association and sedimentation was considered quantitatively, and the information resulting from conservation of mass was used by integration. According to this procedure, the experimental data can be described by an isodesmic association constant of 8 X 10(3) M-1 with satisfactory accuracy. Temperature-jump relaxation detected by fluorescence measurements provides independent evidence for codon-induced association of the anticodon loop. The data are consistent with the following mechanism: UUC preferentially binds to one of two loop conformations with a rate constant of 4.5 X 10(6) M-1 s-1; the UUC-anticodon loop complex undergoes association with a rate constant of 6.5 X 10(6) M-1 s-1. The reactions observed for the isolated anticodon loop are surprisingly similar to those observed previously for the complete tRNA, suggesting that simple hairpin loops are appropriate adaptors for a translation process at an early stage of evolution; the codon-induced association of the hairpin loop should be very useful to facilitate the transfer of cognate amino acids during translation.

Anticodon↗
PubMed1986

Structure and dynamics of double helices in solution: modes of DNA bending.

The long range structure of DNA restriction fragments has been analysed by electro-optical measurements. The overall rotation time constants observed in a low salt buffer with monovalent ions is shown to decrease upon addition of Mg2+ or spermine. Since the circular dichroism and also the limiting value of the linear dichroism remain almost constant under these conditions, the effect is attributed to a change of the long range structure. According to a weakly bending rod model, the persistence length decreases from about 600 A in the absence of Mg2+ or spermine to about 350 A in the presence of these ions. The persistence length measured in the presence of Mg2+ is almost independent of temperature in the range of 10 to 40 degrees C. The nature of DNA bending is analysed by measurements of bending amplitudes and time constants from dichroism decay curves. The observed absence of changes in the bending amplitudes upon addition of Mg2+ or spermine, even though addition induces changes of the persistence length by a factor of 2, is hardly consistent with simple thermal bending. The combined results, including the remarkably small temperature dependence of persistence length and bending amplitude, can be explained by the existence of two bending effects: inherent curvature of DNA dominates at low temperature, whereas thermal bending prevails at high temperature. Analysis of bending amplitudes from dichroism decay curves according to an arc model provides an approximate measure for the degree of bending in restriction fragments. The model is consistent with the observed chain length dependence of bending amplitudes and provides an approximate curvature corresponding to a radius of about 400 A. Thus the curvature observed in restriction fragments is similar to that observed for high molecular DNA condensed into toroids by addition of ions like spermine. Particularly strong bending of DNA is induced by [Co(NH3)6]3+, indicated by an apparent persistence length of 200 A and an increased bending amplitude together with a reduced limit value of the linear dichroism. This effect is attributed to the high charge density of this ion and potential site binding.

DNA, Superhelical↗
PubMed1985

Mechanism of codon recognition by transfer RNA studied with oligonucleotides larger than triplets.

The binding of yeast tRNAPhe to UUCA, UUCC, UUCCC, UUCUUCU, U4, U5, U6 and U7 was analysed by fluorescence temperature jump and equilibrium sedimentation measurements. In all cases the two observed relaxation processes can be assigned to alpha) an intramolecular conformation change of the anticodon loop and beta) preferential binding of the oligonucleotides to one of the anticodon conformations. The anticodon loop transition is associated with inner sphere complexation of Mg2+ and proceeds with rate constants of about 10(3) s-1. The rate constants of oligonucleotide binding are between 4 and 10 X 10(6) M-1s-1 and reflect an increase of the association rate with the number of binding sites compensated to some degree by electrostatic repulsion in the preequilibrium complex. Neither temperature jump nor equilibrium sedimentation experiments provided evidence for UUCA or UUCC induced tRNA dimerisation, although UUC binding leads to strong tRNA dimerisation under equivalent conditions. The results obtained for the longer oligonucleotides are similar. In the case of UUCUUCU with its two potential binding sites for tRNAPhe there was no evidence for the formation of 'ternary' complexes. Apparently tRNAPhe binds preferentially to the second UUC of this 'messenger' and forms additional contacts with residues on either side of the codon. Some evidence for the formation of ternary complexes is obtained for U6 and U7, although the extent of this reaction remains very small. Our results demonstrate that the mode of tRNA binding to a codon is strongly influenced by residues next to the codon. The formation of cooperative contacts between tRNA molecules at adjacent codons apparently requires support by a catalyst adjusting an appropriate conformation of messenger and tRNA molecules.

Anticodon↗
PubMed1985

The mechanism of ion polarisation along DNA double helices.

The orientation curves of short DNA fragments induced by electric field pulses are measured with high time resolution and analysed by efficient deconvolution techniques. A small, but clearly detectable delay of the 'on-field' orientation can be described accurately by the superposition of two exponential processes with opposite amplitudes. The time constant of the faster process is around 10 ns and the slower one in the range 50-1000 ns depending upon the electric field strength and chain length of the DNA fragment. The relation between amplitudes and time constants observed for each curve corresponds exactly to that expected for a convolution of two processes, where the first process is without optical response and becomes detectable only via the optical response of the second process. These results indicate that the first process reflects the polarisation of the ion atmosphere required for the second process of the orientation. Measurements at different ion concentrations c demonstrate that the reciprocal time constant of the fast process is a linear function of c and thus is consistent with an association reaction. The association rate constant evaluated from this dependence according to a simple bimolecular reaction model is 8 X 10(9) M-1 s-1 for a 95 base-pair fragment and is consistent with binding of Na+ to the helix, a reaction close to the limit of diffusion control. The association rate constant is almost independent of the electric field strength E, while the dissociation rate constant k- strongly increases with E, indicating dissociation of ions at high E values. The data suggest a linear correlation between log(k-) and E2 corresponding to a reaction driven by a dipole change. The apparent dipole change evaluated from this dependence is in the order of magnitude estimated for an elementary step of ion dissociation at one end of the helices. The combined results obtained from the polarisation and the orientation mechanism can be explained by dissociation of surprisingly few counterions biased towards one end of the helices. The experimental data obtained for a 76 base-pair fragment are analogous to those for the 95 base-pair fragment, whereas the 'slow' ion polarisation has not been detected for a fragment with 27 base-pairs. This result together with those obtained for the longer fragments at low field strengths indicate that there is a fast polarisation mechanism without 'ion dissociation' at low chain lengths and for low electric field strengths. This mechanism is replaced at high chain lengths and/or high electric field strengths by the ion dissociation mechanism.(ABSTRACT TRUNCATED AT 400 WORDS)

Base Composition↗
PubMed1985

The conformation of single stranded oligonucleotides and of oligonucleotide-oligopeptide complexes from their rotation relaxation in the nanosecond time range.

The conformation of single stranded oligonucleotides is analysed by measurements of their rotation time constants. The oligomers are aligned to some degree by short electric field pulses; after pulse termination the transition to a random orientation is followed by measurements of the linear dichroism. An efficient deconvolution procedure is developed for evaluation of the experimental data obtained in the ns-time range. The increase of rotation time constants observed for chain lengths in the range from 14 to 22 residues are interpreted according to a weakly bending rod model providing a persistence length and a Stokes' diameter. The Stokes' diameters obtained for ribo- and deoxyriboadenylates are about 13A, in approximate agreement with the expectation for a single stranded helix. The persistence length L = 53A corresponding to approximately 16 nucleotide residues found for riboadenylates at 2 degrees C appears to reflect relatively strong stacking interactions at this temperature. However, a comparison with the average length of stacked residues evaluated from available thermodynamic parameters of base stacking indicate that unstacked residues are not completely flexible. Apparently the ribose-phosphate chain provides an essential contribution to the stiffness of oligomers and polymers, even when the bases are unstacked. Addition of 100 microM Mg2+ leads to an increase of the persistence length to 88A. Corresponding measurements with deoxyriboadenylates show a slightly lower value of the persistence length than that found for riboadenylates. Addition of LysTrpLys and LysTyrLys to A(pA)19 leads to an increase of the rotation time constant, which corresponds approximately to a length increment by one residue per bound peptide. Since controls performed with LysLeuLys do not show any similar effect, the increase of the time constants induced by LysTrpLys and LysTyrLys is attributed to intercalation of the aromatic amino acids.

Chemical Phenomena↗
PubMed1984

The change of DNA structure by specific binding of the cAMP receptor protein from rotation diffusion and dichroism measurements.

The structure of complexes formed between cAMP receptor protein (CRP) and various restriction fragments from the promoter region of the lactose operon has been analysed by measurements of electrodichroism. Binding of CRP to a 62-bp fragment containing the major site leads to an increase of the rotation time constant from 0.33 to 0.43 microseconds; addition of cAMP to the complex induces a decrease to 0.25 microseconds. Similar data are obtained for a 80-bp fragment containing the operator site; however, in this case the decrease of the rotation time for the specific complex is only observed when the salt concentration is increased from 3 to 13 mM. A 203-bp fragment containing both sites showed a corresponding change after pre-incubation at 50 mM salt. The salt dependence of the rotation time for the specific complex formed with the 203-bp fragment also indicates that a compact structure is formed at 13 mM salt, whereas the structure is not as compact at 3 mM salt. A 98-bp fragment without specific CRP sites did not reveal changes corresponding to those observed for the specific fragments. The rotation time constants together with the dichroism amplitudes indicate that binding of CRP to specific sites in the presence of cAMP leads to the formation of compact structures, which are consistent with bending of DNA helices. The observed strong salt dependence of the structure is apparently due to electrostatic repulsion between adjoining helix segments.

Base Composition↗