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Dihedrals

J is almost always positive and its magnitude often exceeds that of T. It always depends in a predictable way on the dihedral angle ( ) between the outer two of the tluee bonds in die coupling patliway. Karplus first showed theoretically that T varies to a good approximation as A cos ( ) + B cos ( ), where A and B are constants, and also that A S>B [17]. Flis equation has received wide-ranging... [Pg.1452]

C2 of A3 (degrees) and a dihedral angle with the fluorine atom of 180.0. All parameters given lettered variable names (LI, A1 ete) will be optimized the dihedral angles are given explieitly as these are fixed by synnnetry (the moleeiile is planar). Simple eonstraints ean be imposed by removing parameters from the optimization list. [Pg.2343]

Because densification occurs via tire shrinkage of tliennodynamically unstable pores, densification and microstmcture development can be assessed on tire basis of tire dihedral angle, 0, fonned as a result of tire surface energy balance between tire two solid-vapour and one solid-solid interface at tire pore-grain boundary intersection [, 78, 79 and 80],... [Pg.2770]

Figure C2.11.7. An illustration of tlie equilibrium dihedral angle, 0, fonned by tlie balance of interfacial energies at a pore-grain boundary intersection during solid-state sintering. Figure C2.11.7. An illustration of tlie equilibrium dihedral angle, 0, fonned by tlie balance of interfacial energies at a pore-grain boundary intersection during solid-state sintering.
But the methods have not really changed. The Verlet algorithm to solve Newton s equations, introduced by Verlet in 1967 [7], and it s variants are still the most popular algorithms today, possibly because they are time-reversible and symplectic, but surely because they are simple. The force field description was then, and still is, a combination of Lennard-Jones and Coulombic terms, with (mostly) harmonic bonds and periodic dihedrals. Modern extensions have added many more parameters but only modestly more reliability. The now almost universal use of constraints for bonds (and sometimes bond angles) was already introduced in 1977 [8]. That polarisability would be necessary was realized then [9], but it is still not routinely implemented today. Long-range interactions are still troublesome, but the methods that now become popular date back to Ewald in 1921 [10] and Hockney and Eastwood in 1981 [11]. [Pg.4]

The free energy differences obtained from our constrained simulations refer to strictly specified states, defined by single points in the 14-dimensional dihedral space. Standard concepts of a molecular conformation include some region, or volume in that space, explored by thermal fluctuations around a transient equilibrium structure. To obtain the free energy differences between conformers of the unconstrained peptide, a correction for the thermodynamic state is needed. The volume of explored conformational space may be estimated from the covariance matrix of the coordinates of interest, = ((Ci [13, lOj. For each of the four selected conform-... [Pg.172]

Using this information, the overall free energy change may thus be decomposed into contributions from individual dihedrals. As with all free energy... [Pg.172]

The top part of Fig. 1 shows the time evolution of the central dihedral angle of butane, r (defined by the four carbon atoms), for trajectories... [Pg.228]

Fig. 1. The time evolution (top) and average cumulative difference (bottom) associated with the central dihedral angle of butane r (defined by the four carbon atoms), for trajectories differing initially in 10 , 10 , and 10 Angstoms of the Cartesian coordinates from a reference trajectory. The leap-frog/Verlet scheme at the timestep At = 1 fs is used in all cases, with an all-atom model comprised of bond-stretch, bond-angle, dihedral-angle, van der Waals, and electrostatic components, a.s specified by the AMBER force field within the INSIGHT/Discover program. Fig. 1. The time evolution (top) and average cumulative difference (bottom) associated with the central dihedral angle of butane r (defined by the four carbon atoms), for trajectories differing initially in 10 , 10 , and 10 Angstoms of the Cartesian coordinates from a reference trajectory. The leap-frog/Verlet scheme at the timestep At = 1 fs is used in all cases, with an all-atom model comprised of bond-stretch, bond-angle, dihedral-angle, van der Waals, and electrostatic components, a.s specified by the AMBER force field within the INSIGHT/Discover program.
Fig. 4. The average end-to-end-distance of butane as a function of timestep (note logarithmic scale) for both single-timestep and triple-timestep Verlet schemes. The timestep used to define the data point for the latter is the outermost timestep At (the interval of updating the nonbonded forces), with the two smaller values used as Atj2 and At/A (for updating the dihedral-angle terms and the bond-length and angle terms, respectively). Fig. 4. The average end-to-end-distance of butane as a function of timestep (note logarithmic scale) for both single-timestep and triple-timestep Verlet schemes. The timestep used to define the data point for the latter is the outermost timestep At (the interval of updating the nonbonded forces), with the two smaller values used as Atj2 and At/A (for updating the dihedral-angle terms and the bond-length and angle terms, respectively).
Fig. 10. Differences in potential energy components for the blocked alanine model (for bond length, bond angle, dihedral angle, van der Waals, and electrostatic terms, shown top to bottom) before and after the residual corrections in LIN trajectories at timesteps of 2 fs (yellow), 5 fs (red), and 10 fs (blue). Fig. 10. Differences in potential energy components for the blocked alanine model (for bond length, bond angle, dihedral angle, van der Waals, and electrostatic terms, shown top to bottom) before and after the residual corrections in LIN trajectories at timesteps of 2 fs (yellow), 5 fs (red), and 10 fs (blue).
A set of rules determines how to set up a Z-matrix properly, Each line in the Z-matiix represents one atom of the molecule. In the first line, atom 1 is defined as Cl, which is a carbon atom and lies at the origin of the coordinate system. The second atom, C2, is at a distance of 1.5 A (second column) from atom 1 (third column) and should always be placed on one of the main axes (the x-axis in Figure 2-92). The third atom, the chlorine atom C13, has to lie in the xy-planc it is at a distanc e of 1.7 A from atom 1, and the angle a between the atoms 3-1-2 is 109 (fourth and fifth columns). The third type of internal coordinate, the torsion angle or dihedral r, is introduced in the fourth line of the Z-matiix in the sixth and seventh column. It is the angle between the planes which arc... [Pg.93]

Additional features determine properties such as interatomic distances, bond angles, and dihedral angles from atomic coordinates. Animations of computed vibrational modes from quantum chemistry packages arc also included. http //fiourceforge.nei/projecl /j mol/... [Pg.155]

Vn is often called the barrier of rotation. This is intuitive but misleading, because the exact energetic barrier of a particular rotation is the sum of all V components and other non-bonding interactions with the atoms under consideration. The multiplicity n gives the number of minima of the function during a 360° rotation of the dihedral angle o). The phase y defines the exact position of the minima. [Pg.343]

The Universal Force Field, UFF, is one of the so-called whole periodic table force fields. It was developed by A. Rappe, W Goddard III, and others. It is a set of simple functional forms and parameters used to model the structure, movement, and interaction of molecules containing any combination of elements in the periodic table. The parameters are defined empirically or by combining atomic parameters based on certain rules. Force constants and geometry parameters depend on hybridization considerations rather than individual values for every combination of atoms in a bond, angle, or dihedral. The equilibrium bond lengths were derived from a combination of atomic radii. The parameters [22, 23], including metal ions [24], were published in several papers. [Pg.350]

In order to account for axial and equatorial positions of protons bonded to cyclo-hcxanc-likc rings, Eq, (19) was used, where 1 is an atom three non-rotatablc bonds (totally atoms) away from the proton and belonging to a six-membered ring, and is a dihedral angle in radians (Figure 10.2-6c). [Pg.526]

Figure 10.2.6. Special distance measures for the characterization of proton environments a) distance r and angle a, to double bonds b) distance and angle Oc, to single bonds c) dihedral angle a, to the third bond from the hydrogen atom. Figure 10.2.6. Special distance measures for the characterization of proton environments a) distance r and angle a, to double bonds b) distance and angle Oc, to single bonds c) dihedral angle a, to the third bond from the hydrogen atom.
To carry out ageometry optimization (minimi/atioiT), IlyperCh em starts with a set of Cartesian coordinates for a molecule and tries to find anew set of coordinates with a minimum potential energy. Yon should appreciate that the potential energy surface is very complex, even for a molecule containing only a few dihedral an gles. [Pg.16]

The potential energy of a molecular system in a force field is the sum of individnal components of the potential, such as bond, angle, and van der Waals potentials (equation H). The energies of the individual bonding components (bonds, angles, and dihedrals) are function s of th e deviation of a molecule from a h ypo-thetical compound that has bonded in teraction s at minimum val-n es. [Pg.22]

In this ixpixsen talivc dihedral polenlial, V is the dihedral force con Sian L. n is th e periodicity of th e Fourier terni, Oo is th e ph ase angle, and t ) is ihe dihedral angle. [Pg.25]

You can detect hydroxyl group transitions hy plotting dihedral an gles versn s lime over the course of th e sim n lation. This is the distance history. Grady investigated the distance history of water... [Pg.76]


See other pages where Dihedrals is mentioned: [Pg.138]    [Pg.230]    [Pg.514]    [Pg.1453]    [Pg.2770]    [Pg.2821]    [Pg.52]    [Pg.70]    [Pg.163]    [Pg.165]    [Pg.166]    [Pg.166]    [Pg.167]    [Pg.169]    [Pg.170]    [Pg.172]    [Pg.231]    [Pg.239]    [Pg.247]    [Pg.249]    [Pg.251]    [Pg.336]    [Pg.339]    [Pg.363]    [Pg.10]    [Pg.25]    [Pg.25]    [Pg.77]    [Pg.82]    [Pg.82]   


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Alkyl hydroperoxides dihedral angles

Angle dihedral torsion

Angle dihedral, hydrogen confined

Angles, dihedral angle

Butane dihedral angle

Conformation, molecular dihedral angle

Conformational notation dihedral angles

Constant dihedral angles

Coupling constant dihedral angle dependence

Coupling constant variation with dihedral angle

Coupling constants dependence on dihedral angle

Coupling constants dihedral angle

Coupling constants, and dihedral angles

Dihedral

Dihedral Closed Subsets

Dihedral Closed Subsets of Finite Valency

Dihedral angle

Dihedral angle 3/cccc

Dihedral angle 3/hcch

Dihedral angle Double bond

Dihedral angle deformation energy

Dihedral angle dependence

Dihedral angle distributions

Dihedral angle energy

Dihedral angle equivalents

Dihedral angle fluctuations

Dihedral angle liquid-phase sintering

Dihedral angle method

Dihedral angle restraints

Dihedral angle rotation

Dihedral angle solid-state sintering

Dihedral angle space

Dihedral angle torsions, interactions

Dihedral angle variations

Dihedral angle, 156 Gaussian

Dihedral angle, definition

Dihedral angles <I> and

Dihedral angles Subject

Dihedral angles changes

Dihedral angles conformational search

Dihedral angles deviations from

Dihedral angles distortion

Dihedral angles linkage

Dihedral angles steric effects

Dihedral angles, and

Dihedral angles, polysaccharides

Dihedral axes

Dihedral barriers

Dihedral bond angles

Dihedral driver

Dihedral planes

Dihedral potential

Dihedral space

Dihedral symmetry

Dihedral torsion

Dihedral transitions

Dihedrals, improper

Distance and dihedral angle

Distance and dihedral angle constraints

Ethane dihedral angles

Group dihedral

Hemoglobin dihedral symmetry

Improper dihedral angle

Improper dihedral-angle interaction

Interaction potential dihedral angle

Interbase dihedral angle

Internal dihedral angle, in group compounds

Linkage dihedral angles about

Mirror planes dihedral

Molecular mechanics dihedral angle

Monte Carlo dihedral search

Peptides dihedral angle

Propane dihedral angle

Protein structure dihedral angles

Proteins dihedral angles

Ramachandran dihedral angle

Reflection operation dihedral

Scalar coupling dihedral angle

Strain dihedral angle deformation

Sulfur dihedral angles

Total dihedral groups

Vacuum, dihedral angle

Vicinal coupling dihedral angle dependence

Vicinal couplings, dihedral

Well-Tempered Metadynamics Using Dihedral Angle

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