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Electrons exceptions

WFth all semi-empirical methods, IlyperChem can also perform psendo-RIfF calculations for open -shell systems. For a doublet stale, all electrons except one are paired. The electron is formally divided into isvo "half electron s" with paired spins. Each halfelec-... [Pg.46]

One should compare capabilities to the electron beam X-ray emission methods of Chapter 3. The major difference is the higher lateral resolution with electron beams and the associated mapping capabilides. Another difference is the shorter probing depth possible with electrons, except when compared to the specialized TXRF method. Comparing electron-beam EDS to X-ray/particle EDS or electron-beam WDS to X-ray/particle WDS, the electron beams have poorer detection limits because of the greater X-ray bacl ound associated with electron... [Pg.336]

If a paint film is to prevent this reaction, it must be impervious to electrons, otherwise the cathodic reaction is merely transferred from the surface of the metal to the surface of the film. Organic polymer films do not contain free electrons, except in the special case of pigmentation with metallic pigments consequently it will be assumed that the conductivity of paint films is entirely ionic. In addition, the films must be impervious to either water or oxygen, so that they prevent either from reaching the surface of the metal. [Pg.591]

Ans. The only oxidation state of fluorine in a compound is -1 it is the most electronegative element. (It always has control of any shared electrons, except in the element, F2.)... [Pg.227]

Ans. /3 is a high-energy electron. +/3 is a positron—a particle with the same properties as the electron except for the sign of its charge, which is positive. [Pg.347]

To represent the formation of bonds between atoms, it is convenient to use a system known as electron dot notation. In this notation, the symbol for an element is used to represent the nucleus of an atom of the element plus all of the electrons except those in the outermost (valence) shell. The... [Pg.375]

In order to find a good approximate wave function, one uses the Hartree-Fock procedure. Indeed, the main reason the Schrodinger equation is not solvable analytically is the presence of interelectronic repulsion of the form e2/r. — r.. In the absence of this term, the equation for an atom with n electrons could be separated into n hydrogen-like equations. The Hartree-Fock method, also called the Self-Consistent-Field method, regards all electrons except one (called, for instance, electron 1), as forming a cloud of electric charge... [Pg.4]

Bethe s formula requires that the velocity of the incident particle be much larger than that of the atomic electrons, a condition not easily fulfilled by the K-electrons except in the lightest elements. The required correction, called the shell correction, is denoted by subtracting a quantity C from the stopping number. In the penetration of high-Z material, even L-shell correction may be required. In that case, C denotes the sum total of all shell corrections. The subject of shell correction has been extensively treated by several authors, and various graphs and formulas are available for its evaluation (see, e.g., Bethe andAshkin, 1953). [Pg.17]

A free atom or a radical possesses an odd number of electrons, except atoms of noble gases. T ypically, a valence-saturated molecule has an even number of electrons. Therefore, the reaction of a radical or an atom with a molecule will inevitably give rise to another atom or radical [1-3] ... [Pg.53]

Z] is considered together with its core electrons Nl- This amounts to a corevalence partitioning of atom k in the molecule its valence region now consists of all the electrons except and of all the other nuclei. At this stage it is not taken into account that the other nuclei—those embedded in the valence region of atom k—may possess core electrons of their own. [Pg.36]

The simulation of a heavy ion track structure employs essentially the same methodology as described for energetic electrons except that... [Pg.87]

IR bands of polysilane radical anions and the location of conduction electrons. Except for poly(diarylsilanes), the conduction electron is confined either in the skeleton or in one of the pendant groups. [Pg.639]

When electron densities are calculated for this projection by the expression alread " given, the map shown in Pig. 209 is obtained. Contours are drawn at intervals of one electron, except round the platinum atom, where the interval is 20 electrons. The detail shown in this striking view of the structure is remarkable every atom is clearly resolved, and the positions of atomic centres can be read off with considerable precision. It should be noted that the flat molecule is inclined at 26 5° to the plane of the paper, and is therefore somewhat foreshortened in one direction. [Pg.376]

In order to illustrate the utility of double groups let us consider several examples. Suppose that we have an ion with one d electron in a planar complex. Real examples of this case are represented by complexes of Ou(II) and Ag(II) (where we virtually have one positron, but this behaves as one electron except in the signs of the energies). In each case there will be two states with / values l i = 2 i, namely, J — i and / = . Using 9.3-2, we find that these form bases for the following representations ... [Pg.300]

Figure 3. XPS survey spectra for four samples of the coating. All labeled peaks correspond to Is electrons, except Ca, which is from a 2p electron. Figure 3. XPS survey spectra for four samples of the coating. All labeled peaks correspond to Is electrons, except Ca, which is from a 2p electron.
Octet rule each atom is assigned 8 electrons except H (2) and atoms with d-orbitals... [Pg.2]

Spin-forbidden transitions are possible in other cations with two or more 3d electrons (except Cu2+, 3d9). Thus, in oxygen ligand environments containing Fe2+ ions in octahedral coordination, spin-forbidden transitions also occur in the crystal field spectra, often appearing as weak, sharp peaks in the visible region, in addition to the broad spin-allowed bands located in the near-infrared... [Pg.70]

Draw a single bond (one pair of electron dots or a line) between each pair of connected atoms. Place the remaining electrons around the atoms as unshared pairs. If every atom has an octet of electrons except H, He, Li, and Be, which are atoms with two electrons, the Lewis structure is complete. Shared electrons count towards both atoms. If there are too few electron pairs to do this, draw multiple bonds (two or three pairs of electron dots between the atoms) until an octet is around each atom (except H atoms with two). If there are two many electron pairs to complete the octets with single bonds then the octet rule Is broken for this compound. [Pg.92]

At LSDA, with nonrelativistic ECPs for inner-shell electrons, except for M = C from Reference 153. [Pg.29]

Propagation. Each radical adds monomer to form longer and longer molecules (P-), each having one unpaired electron. Except for the initiator radical, all the radicals are assumed to add monomer with equal reactivity and at a rate which is first order in monomer concentration. [Pg.52]


See other pages where Electrons exceptions is mentioned: [Pg.514]    [Pg.348]    [Pg.557]    [Pg.40]    [Pg.279]    [Pg.358]    [Pg.7]    [Pg.18]    [Pg.317]    [Pg.261]    [Pg.32]    [Pg.129]    [Pg.208]    [Pg.51]    [Pg.334]    [Pg.23]    [Pg.30]    [Pg.183]    [Pg.30]    [Pg.96]    [Pg.170]    [Pg.65]    [Pg.194]    [Pg.12]    [Pg.27]    [Pg.177]    [Pg.178]    [Pg.146]   
See also in sourсe #XX -- [ Pg.5 , Pg.106 ]




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