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Hydrogen atom, calculations

Following the most commonly used approach, that of truncating the cluster with hydrogen atoms, calculations were performed on an Si50i6Hi2 molecule, using a 3-2IG basis set. Four variants of this system were tested, and the... [Pg.72]

Let us now consider the velocity autocorrelation function (VACF) obtained from the MCYL potential, (namely, with the inclusion of vibrations). Figure 3 shows the velocity autocorrelation function for the oxygen and hydrogen atoms calculated for a temperature of about 300 K. The global shape of the VACF for the oxygen is very similar to what was previously determined for the MCY model. Very notable are the fast oscillations for the hydrogens relative to the oxygen. [Pg.246]

The previous section has described how one can compute accurately a system of about 30 atoms including one transition metal. The problem is, as mentioned above, that these are usually not the real catalysts, but model systems where the bulky substituents have been replaced by hydrogen atoms. Calculations on model systems are usually at least indicative of the nature and the energy barriers of the steps involved in a catalytic cycle, but they are often unable to provide information on some of the most interesting features, namely enantioselectivity and regioselectivity. The reason for this failure is simply that selectivity is often associated to the presence of the bulky substituents which are deleted when defining the model system. [Pg.12]

The average distance of the electron from the nucleus in the ground state of hydrogen atom calculated given that the normalized ground state wave function is ... [Pg.156]

The wavelength of light at which the Balmer series converges (Problem 5.45) corresponds to the amount of energy required to completely remove an electron from the second shell of a hydrogen atom. Calculate this energy in kilojoules per mole. [Pg.194]

Figure 21. (X )hp as a function of T for protein hydrogen atoms calculated from MD simulations [74]. Figure 21. (X )hp as a function of T for protein hydrogen atoms calculated from MD simulations [74].
The statistical mechanics of an electron. Calculate the two lowest energy levels for an electron in a box of volume V = 1(This is an approximate model for the hydrogen atom). Calculate the partition function at T = 300 K. Are quantum effects important ... [Pg.217]

Calculate the total electronic energy of a mole of hydrogen atoms. Calculate the total electronic energy of a mole of He atoms. What accounts for the difference in the two total energies ... [Pg.385]

Applications of quantum mechanics to chemistry invariably deal with systems (atoms and molecules) that contain more than one particle. Apart from the hydrogen atom, the stationary-state energies caimot be calculated exactly, and compromises must be made in order to estimate them. Perhaps the most useful and widely used approximation in chemistry is the independent-particle approximation, which can take several fomis. Conuiion to all of these is the assumption that the Hamiltonian operator for a system consisting of n particles is approximated by tlie sum... [Pg.24]

Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold. Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold.
Methane, CH4, for example, has a central carbon atom bonded to four hydrogen atoms and the shape is a regular tetrahedron with a H—C—H bond angle of 109°28, exactly that calculated. Electrons in a lone pair , a pair of electrons not used in bonding, occupy a larger fraction of space adjacent to their parent atom since they are under the influence of one nucleus, unlike bonding pairs of electrons which are under the influence of two nuclei. Thus, whenever a lone pair is present some distortion of the essential shape occurs. [Pg.38]

In the following matrices hydrogen atoms are sometimes not shown, because their numbers and position.s can be calculated from organic structures on the basis of the valence rules of the other atoms. [Pg.34]

Figure 2-44, The EC values of the atoins of phenylalanine (without hydrogens) are calculated by considering the class values of the neighboring atoms, After each relaKatlon process, c, the number of equivalent classes (different EC values), is determined. Figure 2-44, The EC values of the atoins of phenylalanine (without hydrogens) are calculated by considering the class values of the neighboring atoms, After each relaKatlon process, c, the number of equivalent classes (different EC values), is determined.
Here, and Lj are local indices having the form shown in Eq. (5), where lo is a constant characterizing the ith atom (in some cases the atom valence can be used to this end), Nh is the number of attached hydrogen atoms and is the charge density calculated by some fast method such as the Marsili-Gasteiger charge calculation method [7]. [Pg.295]

A second idea to save computational time addresses the fact that hydrogen atoms, when involved in a chemical bond, show the fastest motions in a molecule. If they have to be reproduced by the simulation, the necessary integration time step At has to be at least 1 fs or even less. This is a problem especially for calculations including explicit solvent molecules, because in the case of water they do not only increase the number of non-bonded interactions, they also increase the number of fast-moving hydrogen atoms. This particular situation is taken into account... [Pg.362]


See other pages where Hydrogen atom, calculations is mentioned: [Pg.19]    [Pg.131]    [Pg.339]    [Pg.19]    [Pg.114]    [Pg.159]    [Pg.102]    [Pg.195]    [Pg.195]    [Pg.112]    [Pg.139]    [Pg.416]    [Pg.226]    [Pg.413]    [Pg.231]    [Pg.19]    [Pg.131]    [Pg.339]    [Pg.19]    [Pg.114]    [Pg.159]    [Pg.102]    [Pg.195]    [Pg.195]    [Pg.112]    [Pg.139]    [Pg.416]    [Pg.226]    [Pg.413]    [Pg.231]    [Pg.67]    [Pg.5]    [Pg.24]    [Pg.33]    [Pg.1145]    [Pg.1256]    [Pg.260]    [Pg.366]    [Pg.385]    [Pg.181]    [Pg.47]    [Pg.50]    [Pg.107]    [Pg.141]    [Pg.143]    [Pg.352]    [Pg.360]    [Pg.363]    [Pg.526]    [Pg.46]   


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