Environmental Engineering Reference
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Note that Tc and the lanthanide elements are not involved in figure 8 because γ′ lv0 ( T m )
value of Tc is absent while those of the lanthanide elements are abnormally small possibly
due to the effect of f electrons on γ′ lv0 ( T m ) value. Since the s + d electrons of most lanthanide
elements remain constant, their γ′ lv ( T m ) values hardly change as shown in table 13, and the
corresponding β values thus approach zero. In other words, f electrons hardly work as valence
electrons.
When elements with empty or full filled electrons of second outmost sub-shell are
considered, only the outermost electron layer ( s electron layer) is valence electrons, two
groups of elements exist, namely s = 1 (IA and IB metals) and s = 2 (IIA and IIB metals).
There still exists a linear correlation between γ′ lv0 ( T m ) and γ lv0 ( T m )/ T m as shown in figure 9.
When figure 8 and figure 9 are compared, the β value of metals in groups IIA an IIB with s =
2 is similar to that of Eq. (5.10). However, the β value of metals in groups IA an IB with s = 1
is 30% smaller than that when the period number n ′ remains constant.
Fe
(a)
Ti
Ni
Mn
Co
2
V
Ca
Cr
Sc
K
0
Ru
(b)
Pd
Nb
Rh
2
Mo
Zr
Sr
Y
Rb
0
(c)
Pt
W
Os
Ta
2
Ir
Re
Hf
Ba
Cs
0
0
4
8
12
γ lv ( T m )/ T m ( × 10 -4 J/m 2 -K)
Figure 8. -γ′ lv0 ( T m ) as a function of γ lv0 ( T m )/ T m for (a) the fourth (7), (b) the fifth (∀) and (c) the sixth
(Β) periods A family metals where the solid lines are determined by Eq. (5.10).
As shown in figures 8 and 9, all elements with the sub-shell of ( n ′-1) d are located on the
right of the figure while all elements with the sub-shell of ( n ′-1) p are found on the left of the
figure. When the sub-shell is ( n ′-1) s , the elements are located in the middle or right of the
figure. In addition, as n ′ increases, -γ′ lv0 ( T m ) values decreases linearly. Thus, the electron
orbital movements and valence electron contributions of sub-shells are different for different
orbitals and different n values as temperature increases. From thermodynamic point of view,
the difference of β between figure 9a and figure 8 is induced by different p values in Eq.
(5.10) since the corresponding H v / T m value is systematically larger than that of the transition
metals.
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