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Ionization energies listed

The molecules and their first vertical ionization energies listed (Table 3) supplement those already presented as examples. The parent silylene has been generated by the SiFLt + 2F — SiH2 + 2HF reaction and investigated by photoionization mass spectroscopy, which yields the adiabatic onset value quoted73. Silyl derivatives such as C(SiH3)4 have been thermally decomposed to detect new routes to amorphous,... [Pg.201]

For reactions of this type, the relative reducing powers of the alkali metals can be predicted from the first ionization energies listed in Table 12.9. Since it is much easier to remove an electron from a cesium atom than from a lithium atom, cesium should be the better reducing agent. The expected trend in reducing ability is... [Pg.570]

Table 7.1 Ground configurations and ground states of atoms, listed in increasing order of atomic number Z, and their first ionization energies, E... Table 7.1 Ground configurations and ground states of atoms, listed in increasing order of atomic number Z, and their first ionization energies, E...
Table 5.1 lists some of the atomic properties of the Group 2 elements. Comparison with the data for Group 1 elements (p. 75) shows the substantial increase in the ionization energies this is related to their smaller size and higher nuclear charge, and is particularly notable for Be. Indeed, the ionic radius of Be is purely a notional figure since no compounds are known in which uncoordinated Be has a 2- - charge. In aqueous solutions the reduction potential of... [Pg.111]

Ionization energies of the main-group elements are listed in Figure 6.15. Notice that ionization energy—... [Pg.155]

The Brueckner-reference method discussed in Section 5.2 and the cc-pvqz basis set without g functions were applied to the vertical ionization energies of ozone [27]. Errors in the results of Table IV lie between 0.07 and 0.17 eV pole strengths (P) displayed beside the ionization energies are approximately equal to 0.9. Examination of cluster amplitudes amd elements of U vectors for each ionization energy reveals the reasons for the success of the present calculations. The cluster operator amplitude for the double excitation to 2bj from la is approximately 0.19. For each final state, the most important operator pertains to an occupied spin-orbital in the reference determinant, but there are significant coefficients for 2h-p operators. For the A2 case, a balanced description of ground state correlation requires inclusion of a 2p-h operator as well. The 2bi orbital s creation or annihilation operator is present in each of the 2h-p and 2p-h operators listed in Table IV. Pole strengths are approximately equal to the square of the principal h operator coefiScient and contributions by other h operators are relatively small. [Pg.48]

The two properties listed in Table 27-1 that suggest that Group 1A metals are unlikely to exist as free metals are (1) the low ionization energies, which show how easily the outermost electron can be removed and (2) very negative standard reduction potentials, which indicate that the aqueous ions are not easily reduced to metals and that the free metals are easily oxidized to 1+ cations. [Pg.437]

Table 1 lists publications containing PE spectra or PE-spectroscopic ionization energies of dienes and polyenes defined by... [Pg.178]

FIGURE 8. Regression of observed vertical ionization energies /" on the corresponding HMO xj values for the set of planar polyenes listed in Table 2... [Pg.206]

Bi has the intermediate value of ionization energy of the five elements listed. [Pg.187]

There are four third-shell electrons in each atom of silicon. In Table 10.4, the values for the ionization energies of these four electrons are listed in kJ/mol. Thus, the energy needed to ionize all four electrons from a mole of silicon atoms is given by ... [Pg.190]

Table 2.8 lists several ionization energies notice that all of them are positive. Figure 2.15 depicts the first ionization energies /(i) (as y) for the elements hydrogen to nobelium (elements 1-102) drawn as a function of atomic number (as x). [Pg.71]

From the ionization potential listed in Table 40 it can be seen that substitution of ethylene or benzene by an electron releasing group of the first period lowers the ionization potential. Also, as the energy gap between the ethylene n MO and the substituent pz AO decreases the change in ionization potential increases. Thus, the energy change for F substitution is 0.22 eV while that for OMe substitution is 1.59 eV. [Pg.161]

O The following data lists the ionization energies for a given atom lEi = 738 kj/mol IE2 = 1451 kj/mol IE3 = 7733 kj/mol. Predict the valence electron configuration for this atom, and explain your reasoning. [Pg.158]

List these elements in order of increasing first ionization energies ... [Pg.215]

All of the levels of theory listed in Table 1.1 predict the C-H bond length with accuracy within 1 %. One piece of cheering information from Table 1.1 is that the DFT method predicts this bond length as accurately as the much more computationally expensive CCSD approach. The error in the ionization energy predicted by HF is substantial, but all three of the other methods give better predictions. The higher levels of theory (MP2 and CCSD) give considerably more accurate results for this quantity than DFT. [Pg.25]

Table 6.1 Contributions of the Keesom, Debye, and London potential energy to the total van der Waals interaction between similar molecules as calculated with Eqs. (6.6), (6.8), and (6.9) using Ctotal = Corient + Cind + Cdisp- They are given in units of 10-79 Jm6. For comparison, the van der Waals coefficient Cexp as derived from the van der Waals equation of state for a gas (P + a/V fj (Vm — b) = RT is tabulated. From the experimentally determined constants a and b the van der Waals coefficient can be calculated with Cexp = 9ab/ (47T21V ) [109] assuming that at very short range the molecules behave like hard core particles. Dipole moments /u, polarizabilities a, and the ionization energies ho of isolated molecules are also listed. Table 6.1 Contributions of the Keesom, Debye, and London potential energy to the total van der Waals interaction between similar molecules as calculated with Eqs. (6.6), (6.8), and (6.9) using Ctotal = Corient + Cind + Cdisp- They are given in units of 10-79 Jm6. For comparison, the van der Waals coefficient Cexp as derived from the van der Waals equation of state for a gas (P + a/V fj (Vm — b) = RT is tabulated. From the experimentally determined constants a and b the van der Waals coefficient can be calculated with Cexp = 9ab/ (47T21V ) [109] assuming that at very short range the molecules behave like hard core particles. Dipole moments /u, polarizabilities a, and the ionization energies ho of isolated molecules are also listed.

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Ionization energy

Ionizing energy

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