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Pauli Exclusion Principle violation

Again, for the filled orbitals L = 0 and 5 = 0, so we have to consider only the 2p electrons. Since n = 2 and f = 1 for both electrons the Pauli exclusion principle is in danger of being violated unless the two electrons have different values of either or m. For non-equivalent electrons we do not have to consider the values of these two quantum numbers because, as either n or f is different for the electrons, there is no danger of violation. [Pg.210]

Primary steric effects are due to repulsions between electrons in valence orbitals on atoms which are not bonded to each other. They are believed to result from the interpenetration of occupied orbitals on one atom by electrons on the other resulting in a violation of the Pauli exclusion principle. All steric interactions raise the energy of the system in which they occur. In terms of their effect on chemical reactivity, they may either decrease or increase a rate or equilibrium constant depending on whether steric interactions are greater in the reactant or in the product (equilibria) or transition state (rate). [Pg.636]

Even if the g-density is A -representable, this Q-matrix is not A -representable because its largest eigenvalue exceeds the upper bound N /Q N — Q+ ). (That is, this g-matrix violates the Pauli exclusion principle for g-tuples of electrons.) Approximating the correction term, Tp Jpg[ (]], seems difficult, and neglecting this term would give poor results, although the results improve with increasing Q [2, 10]. [Pg.474]

A common reference density, first used by Roux and Daudel (1955), is the superposition of spherical ground-state atoms, centered at the nuclear positions. It is referred to as the promolecule density, or simply the promolecule, as it represents the ensemble of randomly oriented, independent atoms prior to interatomic bonding. It is a hypothetical entity that violates the Pauli exclusion principle. Nevertheless, the promolecule is electrostatically binding if only the electrostatic interactions would exist, the promolecule would be stable (Hirshfeld and Rzotkiewicz 1974). The difference density calculated with the promolecule reference state is commonly called the deformation density, or the standard deformation density. It is the difference between the total density and the density corresponding to the sum of the spherical ground-state atoms located at the positions R... [Pg.95]

Using the above definitions for the four quantum numbers, we can list what combinations of quantum numbers are possible. A basic rule when working with quantum numbers is that no two electrons in the same atom can have an identical set of quantum numbers. This rule is known as the Pauli Exclusion Principle named after Wolfgang Pauli (1900-1958). For example, when n = 1,1 and mj can be only 0 and m can be + / or -1/ This means the K shell can hold a maximum of two electrons. The two electrons would have quantum numbers of 1,0,0, + / and 1,0,0,- /, respectively. We see that the opposite spin of the two electrons in the K orbital means the electrons do not violate the Pauli Exclusion Principle. Possible values for quantum numbers and the maximum number of electrons each orbital can hold are given in Table 4.3 and shown in Figure 4.7. [Pg.42]

In addition to the Coulombic forces, there is a repulsive force which operates at short distances between ions as a result of the overlapping of filled orbitals, potentially a violation of the Pauli exclusion principle. This repulsive force may be represented by the equation ... [Pg.158]

This bonding scheme permits two pairs of electrons to be shared between two atoms so diat each pair occupies a different region of space and does not violate the Pauli exclusion principle. Since only two p orbitals are used in the hybridization and they are orthogonal and define a plane, the sp2-hybridized carbon is planar with bond angles of 120°. The remaining p orbital, which is left unhybridized to form the n bond, is perpendicular to the molecular plane. Once formed, the n bond keeps the entire system rigid and planar, because rotation of one end of die -bonded system relative to the other end requires diat die it bond be broken. [Pg.11]

The sharing of three pairs of elections between two atoms can be accomplished by extrapolation of die above considerations. That is, since there can only be one o bond connecting the atoms, then die othei two pairs of shared electrons must be in two diffeient tc bonds, each of which is formed by the parallel overlap of a p orbital. Furthermore die n bonds must be mutually orthogonal so as not to violate the Pauli exclusion principle. Hybridization of one s orbital and one p oibital gives two equivalent sp hybiid AOs which are linearly opposite to one anodier. [Pg.11]

The symbol for the normal hydrogen molecule is and means the following (/) there is no net orbital angular momentum around the axis of the molecule (/ /) the two electron spins are paired (as they have to be if the Pauli Exclusion Principle is not to be violated) (iii) the sum of the f s is an even number (zero in this case) and leads to the subscript g, which means that the wave function does not change sign by inversion through the center of symmetry (otherwise the symbol u would be used). [Pg.21]

The Hartree-Fock equations (5.47) (in matrix form Eqs. 5.44 and 5.46) are pseudoeigenvalue equations asserting that the Fock operator F acts on a wavefunction i//, to generate an energy value ,-, times i/q. Pseudoeigenvalue because, as stated above, in a true eigenvalue equation the operator is not dependent on the function on which it acts in the Hartree-Fock equations F depends on i// because (Eq. 5.36) the operator contains J and K, which in turn depend (Eqs. 5.29 and 5.30) on i//. Each of the equations in the set (5.47) is for a single electron ( electron 1 is indicated, but any ordinal number could be used), so the Hartree-Fock operator F is a one-electron operator, and each spatial molecular orbital i// is a one-electron function (of the coordinates of the electron). Two electrons can be placed in a spatial orbital because the, full description of each of these electrons requires a spin function 7 or jl (Section 5.2.3.1) and each electron moves in a different spin orbital. The result is that the two electrons in the spatial orbital i// do not have all four quantum numbers the same (for an atomic Is orbital, for example, one electron has quantum numbers n= 1, / = 0, m = 0 and s = 1/2, while the other has n= l,l = 0,m = 0 and s = —1/2), and so the Pauli exclusion principle is not violated. [Pg.194]

The correct answer is (C). By placing 8 electrons in the 2p orbitals, (C) is in violation of the Pauli exclusion principle, which states that each orbital may only contain 2 electrons and that those must have opposite spins. Eight electrons exceed the maximum six. [Pg.84]

In order for two electrons to occupy the same orbital, they must have oppositely paired spin quantum numbers (denoted as +1/2 and -1/2). Any deviation from this rule violates the Pauli exclusion principle, which states that if two electrons share the same orbital, their spins must be opposed. There is also, another possibility upon promotion of the electron. [Pg.245]

There are also cases in which the unpaired localized electrons of the lattice interact with the conduction electrons. The information of the spin state of a given ion is transmitted to another one, via the conduction electrons. Since the Pauli exclusion principle cannot be violated, the spins, feeling the interaction, will comply. This is called the Ruderman-Kittel interaction. [Pg.274]

The sum over internal lines is unrestricted so (linked) exclusion principle violating (e-v38 or EPV27) terms are included in the sums. Note that either restricting sums to eliminate both unlinked and linked EPV diagrams or unrestricting summations and doing a simple cancellation of unlinked terms satisfies the Pauli exclusion principle.27... [Pg.229]

These data provide two explanations for slow or no reactivity. First, the reactions with 02 must occur by one-electron transfers (eq 1) rather than two s Iectron transfers because the anions cannot donate two electrons to partially rdled 02 orbitals (Figure 2). This scenario would be a violation of the Pauli exclusion principle. [Pg.141]

State the Pauli Exclusion Principle. Would any of the following electron configurations violate this rule (a) Is ... [Pg.231]


See other pages where Pauli Exclusion Principle violation is mentioned: [Pg.175]    [Pg.514]    [Pg.232]    [Pg.140]    [Pg.14]    [Pg.703]    [Pg.202]    [Pg.69]    [Pg.474]    [Pg.674]    [Pg.342]    [Pg.183]    [Pg.218]    [Pg.48]    [Pg.93]    [Pg.293]    [Pg.64]    [Pg.82]    [Pg.478]    [Pg.322]    [Pg.195]    [Pg.633]    [Pg.633]    [Pg.703]    [Pg.92]    [Pg.483]    [Pg.307]   
See also in sourсe #XX -- [ Pg.157 ]




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