I have developed "tennis elbow" from lugging this book around the past four weeks, but it is worth the pain, the effort, and the aspirin. It is also worth the (relatively speaking) bargain price. Including appendixes, this book contains 894 pages of text. The entire panorama of the neural sciences is surveyed and examined, and it is comprehensive in its scope, from genomes to social behaviors. The editors explicitly state that the book is designed as "an introductory text for students of biology, behavior, and medicine," but it is hard to imagine any audience, interested in any fragment of neuroscience at any level of sophistication, that would not enjoy this book. The editors have done a masterful job of weaving together the biologic, the behavioral, and the clinical sciences into a single tapestry in which everyone from the molecular biologist to the practicing psychiatrist can find and appreciate his or

Principles of Neural Science

We have developed novel nucleic acid probes that recognize and report the presence of specific nucleic acids in homogeneous solutions. These probes undergo a spontaneous fluorogenic conformational change when they hybridize to their targets. Only perfectly complementary targets elicit this response, as hybridization does not occur when the target contains a mismatched nucleotide or a deletion. The probes are particularly suited for monitoring the synthesis of specific nucleic acids in real time. When used in nucleic acid amplification assays, gene detection is homogeneous and sensitive, and can be carried out in a sealed tube. When introduced into living cells, these probes should enable the origin, movement, and fate of specific mRNAs to be traced.

Molecular Beacons: Probes that Fluoresce upon Hybridization

IA. Cause and Effect . . . . . . . . . . . . . . 465 1.2. Prerequisites of Selforganization . . . . . . . 467 1.2.3. Evolut ion Must S ta r t f rom R andom Even ts 467 1.2.2. Ins t ruc t ion Requires In format ion . . . . 467 1.2.3. In format ion Originates or Gains Value by S e l e c t i o n . . . . . . . . . . . . . . . 469 1.2.4. Selection Occurs wi th Special Substances under Special Conditions . . . . . . . . 470

/pdf/selforganization-of-matter-and-the-evolution-of-biological-3ms9rkbxjp.pdf

Selforganization of matter and the evolution of biological macromolecules

Although the importance of the polyelectrolyte character of DNA has been recognized for some time (Felsenfeld & Miles 1967), few of the implications have been explored, primarily because of a lag in translating the breakthroughs in polyelectrolyte theory of the last decade into a form that is well adapted to the analysis of the specialized problems of biophysical chemistry. Perhaps an analogous situation existed in the field of protein chemistry during the period after the formulation and confirmation of the Debye—Huckel theory of ionic solutions but before Scatchard's incorporation of the theory into his analysis of the binding properties of proteins. An achievement for polynucleotide solutions parallel to Scatchard's was recently presented by Record, Lohman, & de Haseth (1976) and further developed and reviewed by Record, Anderson & Lohman (1978).

https://www.cambridge.org/core/services/aop-cambridge-core/content/view/S0033583500002031

The molecular theory of polyelectrolyte solutions with applications to the electrostatic properties of polynucleotides.

We report a series of experiments and a theoretical model designed to systematically define and evaluate the relative importance of nanoparticle, oligonucleotide, and environmental variables that contribute to the observed sharp melting transitions associated with DNA-linked nanoparticle structures. These variables include the size of the nanoparticles, the surface density of the oligonucleotides on the nanoparticles, the dielectric constant of the surrounding medium, target concentration, and the position of the nanoparticles with respect to one another within the aggregate. The experimental data may be understood in terms of a thermodynamic model that attributes the sharp melting to a cooperative mechanism that results from two key factors: the presence of multiple DNA linkers between each pair of nanoparticles and a decrease in the melting temperature as DNA strands melt due to a concomitant reduction in local salt concentration. The cooperative melting effect, originating from short-range duplex-to-duplex interactions, is independent of DNA base sequences studied and should be universal for any type of nanostructured probe that is heavily functionalized with oligonucleotides. Understanding the fundamental origins of the melting properties of DNA-linked nanoparticle aggregates (or monolayers) is of paramount importance because these properties directly impact one's ability to formulate high sensitivity and selectivity DNA detection systems and construct materials from these novel nanoparticle materials.

What controls the melting properties of DNA-linked gold nanoparticle assemblies?

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.

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

Model calculations on the kinetics of oligonucleotide double helix coil transitions. Evidence for a fast chain sliding reaction.

A direct measurement of the unzippering rate of a nucleic acid double helix.

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 °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 le...

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

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)

/pdf/the-nature-of-protein-dipole-moments-experimental-and-3jlmh1ohux.pdf

Dietmar Porschke

Papers

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

Model calculations on the kinetics of oligonucleotide double helix coil transitions. Evidence for a fast chain sliding reaction.

A direct measurement of the unzippering rate of a nucleic acid double helix.

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

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