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Filling orbitals

The lowest-energy orbitals fill up fust, according to the order Is —> 2s —> 2p —> 3s —> 3p — 4s — 3d, a statement called the aufbciii principle. Note that the 4s orbital lies between the 3p and 3d orbitals in energy. [Pg.6]

To answer this question, it is necessary to consider the shape or spatial distribution of the orbitals filled by bonding electrons in molecules. From this point of view, we can distinguish between two types of bonding orbitals. Ihe first of these, and by far the more common, is called a sigma bonding orbital. It consists of a single lobe ... [Pg.189]

But I want to return to my claim that quantum mechanics does not really explain the fact that the third row contains 18 elements to take one example. The development of the first of the period from potassium to krypton is not due to the successive filling of 3s, 3p and 3d electrons but due to the filling of 4s, 3d and 4p. It just so happens that both of these sets of orbitals are filled by a total of 18 electrons. This coincidence is what gives the common explanation its apparent credence in this and later periods of the periodic table. As a consequence the explanation for the form of the periodic system in terms of how the quantum numbers are related is semi-empirical, since the order of orbital filling is obtained form experimental data. This is really the essence of Lowdin s quoted remark about the (n + , n) rule. [Pg.100]

Only if shells filled sequentially, which they do not, would the theoretical relationship between the quantum numbers provide a purely deductive explanation of the periodic system. The fact the 4s orbital fills in preference to the 3d orbitals is not predicted in general for the transition metals but only rationalized on a case by case basis as I have argued. Again, I would like to stress that whether or not more elaborate calculations finally succeed in justifying the experimentally observed ground state does not fundamentally alter the overall situation.12... [Pg.100]

Modern ab initio calculations daily confirm the usefulness of the orbital-based quantal perspective as a basis for predicting complex chemical phenomena. In this framework the fundamental descriptors of the orbital filling sequence are the... [Pg.136]

These 20 cases do not represent anomalies to the order of orbital filling which is invariably governed by the n + ( rule but are anomalous in the sense that the s orbital is not completely filled before the corresponding d orbital begins to fill. [Pg.139]

Apparent anomalies in the filling of electron orbitals in atoms occur in chromium and copper. In these elements an electron expected to fill an s-orbital fills the d-orbitals instead, (a) Explain why these anomalies occurs, (b) Similar anomalies are known to occur in seven other elements. Using Appendix 2C, identify those elements and indicate for which ones the explanation used to rationalize the chromium and copper electron configurations is valid, (c) Explain why there are no elements in which electrons fill ( / + I )s-orbitals instead of np-orbitals. [Pg.179]

Which a — 2 orbital does the third electron in a lithium atom occupy Screening causes the orbitals with the same principal quantum number to decrease in stability as / increases. Consequently, the 2 S orbital, being more stable than the 2 orbital, fills first. Similarly, 3 S fills before 3 p, which fills before 3 d, and so on. [Pg.515]

The periodic table provides the answer. Each cut in the ribbon of the elements falls at the end of the p block. This indicates that when the n p orbitals are full, the next orbital to accept electrons is the ( + 1 )s orbital. For example, after filling the 3 orbitals from A1 (Z = 13) to Ar (Z = 18), the next element, potassium, has its final electron in the 4 S orbital rather than in one of the 3 d orbitals. According to the aufbau principle, this shows that the potassium atom is more stable with one electron in its 4 orbital than with one electron in one of its 3 (i orbitals. The 3 d orbitals fill after the 4 S orbital is full, starting with scandium (Z = 21). [Pg.517]

The periodic table in block form, showing the filling sequence of the atomic orbitals. Filling proceeds from left to right across each row and from the right end of each row to the left end of the succeeding row. [Pg.518]

For this qualitative problem, use the periodic table to determine the order of orbital filling. Locate the element in a block and identify its row and column. Move along the ribbon of elements to establish the sequence of filled orbitals. [Pg.518]

Between barium (Group 2, element 56) and lutetium (Group 3, element 71), the 4f orbitals fill with electrons, giving rise to the lanthanides, a set of 14 metals named for lanthanum, the first member of the series. The lanthanides are also called the rare earths, although except for promethium they are not particularly rare. Between radium (Group 2, element 88) and lawrenclum (Group 3, element 103), are the 14 actinides, named for the first member of the set, actinium. The lanthanides and actinides are also known as the inner transition metals. [Pg.1430]

Explain the relevance of atomic orbital overlap and of molecular orbital filling to the strength of the bond formed between two atoms. [Pg.408]

Aufbau principle The principle that states that the lowest-energy orbitals fill first when electrons are added to successive elements in the periodic table. [Pg.117]

Halide ions have lower orbitals filled in a rare gas configuration. Their reaction rates with eh are expected to be small, which is verified experimentally. I, I , and CIO-, however, react with e, at near diffusion-controlled rates. [Pg.184]

A state for which / = 1 is known as a p state, so the six sets of quantum numbers just shown belong to the 2p state. Population of the 2p state is started with boron and completed with neon in the first long period of the periodic table. However, each m value denotes an orbital, so there are three orbitals where electrons can reside. Electrons remain unpaired as long as possible when populating a set of orbitals. For convenience, we will assume that the orbitals fill by starting with the highest positive value of m first and then going to successive lower values. Table 2.3 shows the maximum population of states based on the value for /. [Pg.53]

As emphasized by Bent, the LST properly places H and He with the s block and realigns file l shells into the actual sequence of configurational orbital filling. The LST therefore avoids the curious STT-based implication that the d-block elements (i = 2) are somehow the transition between the s block (l = 0) and p block (l = 1). [Pg.717]

At this point, you re usually given the temperature versus mole fraction diagram for two miscible liquids (Fig. 140), and you re told it s a consequence of Raoult s Law. Well, yes. But not directly. Raoult s Law is a relationship of pressure, not temperature, versus mole fraction and Raoult s Law is pretty much a straight line. You don t need all your orbitals filled to see that you ve been presented with a temperature versus mole fraction diagram, there are two lines (not one), and neither of them are very straight. [Pg.295]

The exceptions begin with the fourth energy level. The fourth energy level begins to fill before all the sublevels in the third shell are complete. More complications in the sequence appear as the value of the principle quantum number increases. The sequence of orbital filling, with complications, is Is, 2s, 2p, 3s, 3p, 4s, 3d, 4p, 5s, 4d, 5p, 6s, 4f, 5d, 6p, 7s, 5f, 6d, and so on. [Pg.112]

Elements that appear in the d block are called the transition elements. They mark the transition from the p orbital filling order to the d orbital filling order. By the same reasoning, the /block elements are called the inner transition elements, because they mark a transition from the d orbital filling order to the / orbital filling order. [Pg.148]

The d block includes all the transition elements. In general, atoms of d block elements have filled ns orbitals, as well as filled or partially filled d orbitals. Generally, the ns orbitals fill before the (n - l)d orbitals. However, there are exceptions (such as chromium and copper) because these two sublevels are very close in energy, especially at higher values of n. Because the five d orbitals can hold a maximum of ten electrons, the d block spans ten groups. [Pg.149]

The /block includes all the inner transition elements. Atoms of /block elements have filled s orbitals in the outer energy levels, as well as filled or partially filled 4/and 5/orbitals. In general, the notation for the orbital filling sequence is ns, followed by (n - 2)/, followed by (n - l]d, followed by (for period 6 elements) np. However, there are many exceptions that make it difficult to predict electron configurations. Because there are seven/orbitals, with a maximum of fourteen electrons, the /block spans fourteen groups. [Pg.149]

The orbits are dense in a state space region i.e. the orbits fills the phase space zone of the strange attractor fl. [Pg.249]

Figure 9 indicates that chemical substitutions which oxidize Mn stabilize the layered structure against transformation only up to a point. At valences higher than +4, i.e., tetrahedral Mn orbital fillings less than d, the trend abruptly shifts (Figure 9). Although in reality such valences are rare for Mn in ccp oxides, Mn is predicted to become less stable in the layered octahedral sites with valences increasing above +4. Figure 9 indicates that chemical substitutions which oxidize Mn stabilize the layered structure against transformation only up to a point. At valences higher than +4, i.e., tetrahedral Mn orbital fillings less than d, the trend abruptly shifts (Figure 9). Although in reality such valences are rare for Mn in ccp oxides, Mn is predicted to become less stable in the layered octahedral sites with valences increasing above +4.
Figures 9—13 show that the energy difference between structures with and without tetrahedral Mn is approximately a linear function of d-orbital filling on the tetrahedral Mn within certain ranges. Figures 9—13 show that the energy difference between structures with and without tetrahedral Mn is approximately a linear function of d-orbital filling on the tetrahedral Mn within certain ranges.
The different regimes that occur as a function of the tetrahedral Mn d-orbital filling (d are as follows. [Pg.285]


See other pages where Filling orbitals is mentioned: [Pg.531]    [Pg.9]    [Pg.12]    [Pg.43]    [Pg.98]    [Pg.1017]    [Pg.517]    [Pg.517]    [Pg.518]    [Pg.49]    [Pg.52]    [Pg.238]    [Pg.238]    [Pg.717]    [Pg.151]    [Pg.21]    [Pg.49]    [Pg.142]    [Pg.331]    [Pg.146]    [Pg.148]    [Pg.149]    [Pg.279]    [Pg.285]    [Pg.285]   
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See also in sourсe #XX -- [ Pg.561 , Pg.562 , Pg.563 , Pg.564 , Pg.565 , Pg.566 , Pg.567 , Pg.570 ]

See also in sourсe #XX -- [ Pg.212 , Pg.233 , Pg.283 ]




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Atomic orbital filling

Atomic orbital filling order

Atomic orbitals filling

Atomic orbitals order of filling

Attraction between molecules filled and empty orbitals

Copper orbital filling order

D orbitals filling

Filled molecular orbitals

Filled orbital of the

Filling of antibonding orbitals

Filling the 2p Orbitals

Filling the 3s, 3p, and 4s Orbitals

Molecular orbital filled

Molecular orbital filling

Orbital filling

Orbital filling process

Orbital highest filled

Orbital interactions filled with unfilled

Orbitals filled

Orbitals filled

Orbitals filling order

Orbitals half-filled

Orbitals orbital filling

Orbitals orbital filling

P orbitals filling

Partially Filling d-Orbitals

Partly filled d-orbitals

S orbitals filling

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