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CHAPTER SEVEN
Periodic Properties of the Elements
Effective nuclear charge, Zeff.
We can estimate the attractive force between any one electron and the
nucleus by considering how the electron interacts with the average
environment created by the nucleus and the other electrons in the atom.
General Chemistry A: First
2013/2014
Zeff. is smaller than the actual nuclear charge (Z ) because the effective nuclear charge
includes the effect of the other electrons in the atom.
Zeff = Z - S
S: Screen outer most electrons from the attraction of the nucleus,
S is a positive number called the screening constant.
the value of S is usually close to the number of core electrons in an atom. (Electrons
in the same valence shell do not screen one another very effectively, but they do
affect the value of S slightly.
For example: Na: [Ne] 3s1. The nuclear charge is Z = 11+ , and there are 10 core
electrons (1s22s22p6). Zeff = 11 - 10 = 1+
Calculation of Zeff by Slater’s rules
Electrons for which the principal quantum number nis larger than the value of n
for the electron of interest. S = 0.
Ignore ‫ تجاهل‬the contribution of an electron to itself in screening;
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Electrons with the same value of n as the electron of interest. S = 0.35
Electrons for which n is 1 less than n for the electron of interest. S = 0.85.
Electrons with even smaller values of n. S = 1.00.
For example, the screening of the valence electron of fluorine atom , 9F : 1s22s22p5, Using
Slater’s rules: S = (6 × 0.35) + ( 2 ×0.85) = 3.8.
Ignore the contribution of an electron to itself in screening;
Zeff = Z - S = 9 - 3.8 = 5.2+
In the case of the alkali metals, Zeff increases from +1.3 for lithium, to + 2.5 for sodium, to
+3.5 for potassium.
Sizes of Atoms and Ions
The bonding atomic radius (the bonding radius): is equal to half of the
nucleus-to nucleus distance d.
The bonding atomic radius
For example, the I2 molecule,
the distance separating the nuclei of I2, (d) = 2.66 Å,
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 The bonding atomic radius of an iodine atom is (2.66 Å)/2 = 1.33 Å.
The C atom, the distance separating the adjacent carbon nuclei in diamond is 1.54 Å;
 The bonding atomic radius of the carbon atom is 0.77 Å.
(For helium and neon, the bonding atomic radii must be estimated because there are no
known compounds of these elements.)
The nonbonding atomic radius or (the van der Waals radius): The shortest distance
separating the two nuclei during the collisions of two atoms is twice the radii of the atoms.
Knowing atomic radii allows us to estimate bond lengths in molecules. For example, the bond
length in Cl2 is 1.99 Å, so a bonding atomic radius of 0.99 Å is assigned to Cl. In CCl4 the
measured length of the bond C  Cl is 1.77 Å, very close to the sum (0.77 + 0.99 Å) of the
bonding atomic radii of C and Cl.
IONIZATION ENERGY
The ionization energy of an atom or ion is the minimum energy required to remove an
electron from the ground state of the isolated gaseous atom or ion.
The first ionization energy, I1, is the energy needed to remove the first electron from
a neutral atom. For example, the first ionization energy for the sodium atom is the
energy required for the process:
Na(g)
Na+(g) + eThe second ionization energy, I2, is the energy needed to remove the second electron,
and so forth, for successive removals of additional electrons.
Thus, I2 for the sodium atom is the energy associated with the process
Na+ (g)
Na2+(g) + eThe greater the ionization energy, the more difficult it is to remove an electron.
I1 < I2 < I3
Periodic Trends in First Ionization Energies
1. The first ionization energy (I1) generally increases as we move across a period. The alkali
metals show the lowest
ionization energy in each period, and the noble gases show the highest. There
are slight irregularities in this trend.
generally decreases as we move down any column in the periodic table. For example,
the ionization energies of the noble gases follow the order: He > Ne > Ar > Kr > Xe.
2. I1
3. The s- and p-block elements show a larger range of I1 values than do the transition metal
elements. Generally, the ionization energies of the transition metals increase slowly from left
to right in a period.
The f-block metals (not shown in Figure 7.9) also show only a small variation in the values of
I1.
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ELECTRON AFFINITIES
The energy change that occurswhen an electron is added to a gaseous atom. It is
a measure of attraction, or affinity, of the atom for the added electron.
For most atoms, energy is released when an electron is added. For example, the
addition of an electron to a chlorine atom is accompanied by an energy change
of the negative sign indicating that energy is released during the process.
Cl (g) + e - → Cl-(g)
∆E = -349 kJ/mol [7.5]
The greater the attraction between an atom and an added electron, the more negative
the atom’s electron affinity.
For some elements, such as the noble gases, the electron affinity has a positive value, which
means that the anion is higher in energy than are the separated atom and electron:
Ar(g) + e - → Ar -(g)
∆E > 0 [7.6]
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The halogens, which are one electron shy of a filled p subshell, have the most negative
electron affinities. By gaining an electron, a halogen atom forms a
stable anion that has a noble-gas configuration (Equation 7.5).
The addition of an electron to a noble gas, however, requires that the electron reside in a
higher-energy subshell that is empty in the atom (Equation 7.6).
Because occupying a higher-energy subshell is energetically unfavorable, the electron affinity
is highly positive.
The electron affinities of Be and Mg are positive for the same reason; the added electron
would reside in the empty p subshell that is higher in energy.
The electron affinities of the group 5A elements are also interesting, since these elements
have half-filled p subshells, the added electron must be put in an orbital that is already
occupied, resulting in a larger electron–electron repulsions. Consequently, these elements
have electron affinities that are either positive (as in N ) or less negative than the electron
affinities of their neighbors to the left (P, As, Sb).
Electron affinities do not change greatly as we move down a group (Figure 7.11).
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‫ مع التركيز على‬، ‫) دراسة ذاتية‬277-264 ‫ (الصفحات‬7.6, 7.7 nd 7.8 :‫تدرس الفقرات التالية‬
(Examples 7.8,7.9 and 7.10 ) ‫األمثلة المذكورة قي الكتاب المقرر‬
METALS, NON METALS, AND METALLOIDS
Characteristic properties of metals and nonmetals
Metals
Have a shiny luster; various colors, although
most are silvery
Solids are malleable and ductile
Nonmetals
Do not have a luster; various colors
Solids are usually brittle; some are hard,
some are soft
Poor conductors of heat and electricity
Good conductors of heat and electricity
Most metal oxides are ionic solids that are
basic
Tend to form cations in aqueous solution
Most nonmetal oxides are molecular
substances
Tend to form anions or oxyanions in aqueous
solution
metallic character generally increases as we proceed down a group of the periodic table and
decreases as we proceed right across a period.
Metals: Metals tend to have low ionization energies (Figure 7.9) and therefore tend to form
cations relatively easily. As a result, metals are oxidized (lose electrons) when they undergo
chemical reactions. Among
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Compounds made up of a metal and a nonmetal tend to be ionic substances. For example,
most metal oxides and halides are ionic solids.
2 Ni(s) + O2(g)
→
2 NiO(s)
[7.7]
Most metal oxides are basic. Those that dissolve in water react to form metal hydroxides,
as in the following examples:
Metal oxide + water
metal hydroxide
Na2O(s) + H2O(l)
2 NaOH(aq)
[7.8]
Metal oxide + acid
NiO(s) + 2 HNO3(aq)
salt + water
Ni(NO3)2(aq) + H2O(l)
[7.11]
NONMETALS
Because of their relatively large, negative electron affinities, nonmetals tend to gain electrons
when they react with metals.
A nonmetal will gain enough electrons to fill its outermost occupied p subshell, giving a
noble-gas electron configuration.
For example, the bromine atom gains one electron to fill its 4p subshell:
Br ([Ar]4s2 3d104p5) + eBr- ([Ar]4s3d104p6)
Compounds composed entirely of nonmetals are typically molecular substances that tend to
be gases, liquids, or low-melting solids at room temperature.
METALLOIDS
Metalloids have properties intermediate between those of metals and those of nonmetals.
Several metalloids, (such as silicon) are electrical semiconductors and are the principal
elements used in integrated circuits and computer chips.
One of the reasons metalloids can be used for integrated circuits is that their electrical
conductivity is intermediate between that of metals and that of nonmetals. Very pure silicon is
an electrical insulator, but its conductivity can be dramatically increased with the addition of
specific impurities called dopants. This modification provides a mechanism for controlling
the electrical conductivity by controlling the chemical composition.
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