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Based on Molecular Fields

Using CoMFA,currently one of the most popular 3D-QSAR techniques, Kim examined the relationships between lipophilicity indices (log P and log k) and various molecular fields (i.e., steric, electrostatic, and hydrogen bond fields). Because the complex nature of lipophilicity was largely [Pg.282]

In our opinion, such approaches are not suitable to calculate log P values from 3D structures for two main reasons  [Pg.283]

A preliminary CoMFA model for a structurally highly diverse series is needed to estimate lipophilicity parameters of new compounds. So far, no heterogeneous series has been reported that could lead to a general predictive CoMFA model for log P calculations. [Pg.283]

The calculation of log P using CoMFA is largely dependent on the position of the solute in the grid used to compute molecular fields. A general CoMFA model implies common alignment rules for diverse solutes, but such rules would presumably be difficult to obtain. [Pg.283]

The molecular lipophilicity potential is a transformation of log Fo tanoi/watcr values (conceptually one-dimensional representations) into three-dimensional representations.The MLP describes the combined lipophilic influence of all fragments in a molecule on its environment and can be calculated at any given point in space around a molecule. Two components are needed to calculate a lipophilicity potential a fragmental system of lipophilicity22.86.95,us g d a distance function, as expressed by the following general equation  [Pg.283]


Fig. 24. Spontaneous magnetization vs. temperature for three ferrogarnets. (After Bertaut and Pauthenet (60). Theoretical curve is based on molecular field parameters obtained by Al mard (5).)... Fig. 24. Spontaneous magnetization vs. temperature for three ferrogarnets. (After Bertaut and Pauthenet (60). Theoretical curve is based on molecular field parameters obtained by Al mard (5).)...
Fig. 28. Paramagnetic susceptibilities of (a) yttrium and (b) gadolinium ferrogarnets. Solid lines are theoretical curves based on molecular field model and empirically determined molecular field constants. Dashed lines are experimental curves indicating effects of short-range order in the neighborhood of the Curie temperature. (After A16onard (5).)... Fig. 28. Paramagnetic susceptibilities of (a) yttrium and (b) gadolinium ferrogarnets. Solid lines are theoretical curves based on molecular field model and empirically determined molecular field constants. Dashed lines are experimental curves indicating effects of short-range order in the neighborhood of the Curie temperature. (After A16onard (5).)...
Ohkoshi, S., Abe, Y., Fujishima, A. and Hashimoto, K. (1999) Design and preparation of a novel magnet exhibiting two compensation temperatures based on molecular field theory. /. Phys. Rev. Lett., 82, 1285-1288. [Pg.208]

The representation of molecular properties on molecular surfaces is only possible with values based on scalar fields. If vector fields, such as the electric fields of molecules, or potential directions of hydrogen bridge bonding, need to be visualized, other methods of representation must be applied. Generally, directed properties are displayed by spatially oriented cones or by field lines. [Pg.137]

It should be noted that a comprehensive ELNES study is possible only by comparing experimentally observed structures with those calculated [2.210-2.212]. This is an extra field of investigation and different procedures based on molecular orbital approaches [2.214—2.216], multiple-scattering theory [2.217, 2.218], or band structure calculations [2.219, 2.220] can be used to compute the densities of electronic states in the valence and conduction bands. [Pg.63]

There are two major theories of bonding in d-metal complexes. Crystal field theory was first devised to explain the colors of solids, particularly ruby, which owes its color to Cr3+ ions, and then adapted to individual complexes. Crystal field theory is simple to apply and enables us to make useful predictions with very little labor. However, it does not account for all the properties of complexes. A more sophisticated approach, ligand field theory (Section 16.12), is based on molecular orbital theory. [Pg.799]

The field of modified electrodes spans a wide area of novel and promising research. The work dted in this article covers fundamental experimental aspects of electrochemistry such as the rate of electron transfer reactions and charge propagation within threedimensional arrays of redox centers and the distances over which electrons can be transferred in outer sphere redox reactions. Questions of polymer chemistry such as the study of permeability of membranes and the diffusion of ions and neutrals in solvent swollen polymers are accessible by new experimental techniques. There is hope of new solutions of macroscopic as well as microscopic electrochemical phenomena the selective and kinetically facile production of substances at square meters of modified electrodes and the detection of trace levels of substances in wastes or in biological material. Technical applications of electronic devices based on molecular chemistry, even those that mimic biological systems of impulse transmission appear feasible and the construction of organic polymer batteries and color displays is close to industrial use. [Pg.81]

A, B and V are constant for a given solute (Eig. 12.4 shows the value of A, 0.78, for atenolol). This means that the balance between intermolecular forces varies with the system investigated as would be expected from a careful reading of Section 12.1.1.3. This can also be demonstrated by using a completely different approach to factorize log P, i.e. a computational method based on molecular interaction fields [10]. Volsurf descriptors [11] have been used to calculate log P of neutral species both in n-octanol-water and in alkane-water [10]. [Pg.323]

Chromophores with a rather high optical anisotropy are the merocyanines (77), especially in the cyanine limit with equal contributions of the apolar and zwitterionic resonance structures [319]. Thus, they also have been proposed as promising candidates for photorefractive systems based on molecular glasses. For 77, doped with a photosensitizer, a refractive index modulation of 0.01 at an electrical field of 22 V/pm was reported. [Pg.163]

The various types of successful approaches can be classified into two groups empirical model calculations based on molecular force fields and quantum mechanical approximations. In the first class of methods experimental data are used to evaluate the parameters which appear in the model. The shape of the potential surfaces in turn is described by expressions which were found to be appropriate by semiclassicala> or quantum mechanical methods. Most calculations of this type are based upon the electrostatic model. Another more general approach, the "consistent force field method, was recently applied to the forces in hydrogen-bonded crystals 48> 49>. [Pg.14]

This chapter will introduce the field of sensors based on molecular imprinted polymers (MIPs). MIPs are highly cross-finked polymers that are formed with the presence of a template molecule (Haupt and Mosbach 2000 Wulff 2002). The removal of the template molecule from the polymer matrix creates a binding cavity that is complementary in size and shape to the template molecule and is fined with appropriately positioned recognition groups (Scheme 15.1). [Pg.395]

On this restricted basis, transition metal phosphines have been modeled with accuracies similar to those of other metal-heteroatom systems11531. A number of phosphine complexes are of interest in the area of asymmetric syntheses. Due to the requirement that the geometry and the force field of the relevant intermediates have to be known for a thorough study (see Chapter 7, Section 7.4) most of the reports in this area are only of a qualitative nature. Some of the investigations are based on molecular graphics analyses, and the evaluation of the predicted selectivity has been based on van der Waals terms alone[53,233,2341. [Pg.136]

Ehrenfest s concept of the discontinuities at the transition point was that the discontinuities were finite, similar to the discontinuities in the entropy and volume for first-order transitions. Only one second-order transition, that of superconductors in zero magnetic field, has been found which is of this type. The others, such as the transition between liquid helium-I and liquid helium-II, the Curie point, the order-disorder transition in some alloys, and transition in certain crystals due to rotational phenomena all have discontinuities that are large and may be infinite. Such discontinuities are particularly evident in the behavior of the heat capacity at constant pressure in the region of the transition temperature. The curve of the heat capacity as a function of the temperature has the general form of the Greek letter lambda and, hence, the points are called lambda points. Except for liquid helium, the effect of pressure on the transition temperature is very small. The behavior of systems at these second-order transitions is not completely known, and further thermodynamic treatment must be based on molecular and statistical concepts. These concepts are beyond the scope of this book, and no further discussion of second-order transitions is given. [Pg.239]


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