quantum mechanics and 2 the chemical bondgriessen/vanquantumtotmaterie/lecturein... · 2006. 12....
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1
Quantum Mechanics and the Chemical Bond
vrije Universiteit amsterdam
Pyrite FeS2
Quartz SiO2
n=1
n=4n=3
n=2
n=5
1,2,3.......1
, 1, 2,....
nl nm l l l l
=≤ −= − − −
The s-wave (l =0) and p-waves (l =1) of the H-atom
+- +
+ --
The d-waves (l =2) of the H atom
+ ++- -
-+
++- -
+
+- -+
+-
-
2
E&R 391
p-states; l=1
d-states; l=2
Chemical bonding in H2+
rL
d
rR
The H2+ molecule-ion (E&R 505-514)
( ) ( )2
, , , ,4 o
e x y z E x y zdψ ψ
πε+ =Proton-proton
repulsion
( ) ( )2 2
, , , ,4 4o L o R
e ex y z x y zr rψ ψ
πε πε− −Proton-electron
attraction
( )2 2 2 2
2 2 2 , ,2
x y zm x y z
ψ⎛ ⎞∂ ∂ ∂
− + +⎜ ⎟∂ ∂ ∂⎝ ⎠Kinetic energy of the electron rL
d
rR
The H2+ molecule-ion
( )
( ) ( )
( ) ( )
2 2 2 2
2 2 2
2 2
2
, ,2
, , , ,4 4
, , , ,4
o L o R
o
x y zm x y z
e ex y z x y zr r
e x y z E x y zd
ψ
ψ ψπε πε
ψ ψπε
⎛ ⎞∂ ∂ ∂− + +⎜ ⎟∂ ∂ ∂⎝ ⎠
− −
+ =
H2+ molecule-ion: simpler notation
L R( )
( ) ( )
( ) ( )
2 2 2 2
2 2 2
2 2
2
, ,2
, , , ,4 4
, , , ,4
o L o R
o
x y zm x y z
e ex y z x y zr r
e x y z E x y zd
ψ
ψ ψπε πε
ψ ψπε
⎛ ⎞∂ ∂ ∂− + +⎜ ⎟∂ ∂ ∂⎝ ⎠
− −
+ =
L R ppT V V V Eψ ψ ψ ψ ψ− − + = L R ppT V V V Eψ ψ ψ ψ ψ− − + =
H2+ molecule-ion: simpler notation
L R
1 1
a H sa b H sbc c
aL bRψ φ φ= +
= +
Probability density cannot depend on what is chosen as left and right
2 2
2 2 2 2
2 2 2 2
22
aL bR
a L abLR b Rb L baLR a R
ψ = +
= + +
= + +2 2 or a b a b a b= ⇒ = = −
3
L R ppT V V V Eψ ψ ψ ψ ψ− − + =
H2+ molecule-ion: normalisation
L R
( )( )
g g
u u
c L R
c L R
ψ
ψ
= +
= −
( )( )
2 2 2 2
2
2
1 2 1 1
d c L LR R d
c S
ψ τ τ= ± +
= ± + =
∫ ∫
1 1 ; 2 2 2 2g uc c
S S= =
+ −
L R ppT V V V Eψ ψ ψ ψ ψ− − + =
H2+ molecule-ion: bonding state
( )g gc L Rψ = +
( )L R ppT V V V Eψ ψ− − + =
( )*L R pp
*
T V V V d
E d E
ψ ψ τ
ψ ψ τ
− − + =
= =
∫∫
As the wave function is normalised
we need only to calculate
( )*L R ppT V V V dψ ψ τ− − +∫ with
H2+ molecule-ion: bonding state
( )g gc L Rψ = +( )*L R ppT V V V dψ ψ τ− − +∫ with
( )( )( )2L R ppT V V VgE c L R L R dτ= + − − + +∫
( )( )( )( )( )( )( )
L R pp
L R pp
L R pp
T V V V
T V V V
T V V V
L R L R d
L R Ld
L R Rd
τ
τ
τ
+ − − + + =
+ − − + +
+ − − + +
∫∫∫
( )( ) ( )( )( )( )( )( )( )
L R pp
1
R
pp
T V V V
V
V
s
L R Ld L R Ld
L R E Ld
L R Ld
L R Ld
τ τ
τ
τ
τ
= + − + + − + =
= + +
+ + −
+ +
∫ ∫∫∫∫
H2+ molecule-ion: bonding state
( )( )L R ppT V V VL R Ldτ+ − − +∫
( )
( )
1
pp
1
V 1
sS EJ K
S
+
− −
+ +
H2+ molecule-ion: bonding state
( )( )( ) ( )
L R pp
1 pp
T V V V
1 V 1s
L R Ld
S E J K S
τ+ − − + =
= + − − + +∫
( ) ( )
( ) ( )
21 pp
1 pp
1 pp
2 1 V 1
1 1 V 11
V1
bonding g s
s
bonding g s
E c S E J K S
S E J K SS
J KE E ES
⎡ ⎤= + − − + + =⎣ ⎦
⎡ ⎤= + − − + + =⎣ ⎦++
= = + −+
Definitions
1 ppV1bonding sJ KE E
S+
= + −+
2
ppV4 o
edπε
= R LS dφ φ τ= ∫
2
4R Ro L
eJ dr
φ φ τπε−
= −∫Coulomb integral
2
4R Lo L
eK dr
φ φ τπε−
= −∫
Exchange integral
4
H2+ molecule-ion: antibonding state
( )( )( ) ( )
L R pp
1 pp
T V V V
1 V 1s
L R Ld
S E J K S
τ+ − − + =
= − − + + −∫
( ) ( )
( ) ( )
21 pp
1 pp
1 pp
2 1 V 1
1 1 V 11
V1
antibonding u s
s
antibonding u s
E c S E J K S
S E J K SS
J KE E ES
⎡ ⎤= − − + + − =⎣ ⎦
⎡ ⎤= − − + + − =⎣ ⎦−−
= = + −−
H2+ molecule-ion: compensation
1 pp
1 pp
V1 1
V1 1
antibonding s
bonding s
J KE ES S
J KE ES S
= + − +− −
= + − −+ +
L R
Proton-proton repulsion is
approx. compensated by proton-electron
attraction
1
1
s
s
E K
E K
≅ +
≅ −
E1s
( )12
L R−
1sE K≅ +
( )12
L R+
1sE K≅ −
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ
Φ=exp(-sqrt( (x-1)^2+y^2))+exp(-sqrt( (x+1)^2+y^2))
Y
X
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ
Φ=exp(-sqrt( (x-1)^2+y^2))-exp(-sqrt( (x+1)^2+y^2))
Y
X
( )12
L R−
( )12
L R+
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ2
IΦI2=(exp(-sqrt( (x-1)^2+y^2))+exp(-sqrt( (x+1)^2+y^2)))^2
Y
X
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ2
IΦI2=(exp(-sqrt( (x-1)^2+y^2))-exp(-sqrt( (x+1)^2+y^2)))^2
Y
X
( )212
L R−
( )212
L R+
Wave function Probability density
E&R page 512
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ
Φ=exp(-sqrt( (x-1)^2+y^2))+exp(-sqrt( (x+1)^2+y^2))
Y
X
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ
Φ=exp(-sqrt( (x-1)^2+y^2))-exp(-sqrt( (x+1)^2+y^2))
Y
X
( )12
L R−
( )12
L R+
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ2
IΦI2=(exp(-sqrt( (x-1)^2+y^2))+exp(-sqrt( (x+1)^2+y^2)))^2
Y
X
-20
2
-1.0-0.8-0.6-0.4-0.20.00.20.40.60.81.01.21.41.6
-2
0
2
Φ2
IΦI2=(exp(-sqrt( (x-1)^2+y^2))-exp(-sqrt( (x+1)^2+y^2)))^2
Y
X
0
0.1
0.2
0.3
0.4
0.5
0.6
-3 -2 -1 1 2 3x
0
0.1
0.2
0.3
0.4
0.5
0.6
-3 -2 -1 1 2 3x
Closer look at the probability density
5
E&R 512-513
Wave function
Probability amplitude
-10 -8 -6 -4 -2 0 2 4 6 8 10-4
-20
24
-2.0
-1.5
-1.0
-0.5
0.0
Pote
ntia
l
Y
X
-10 -8 -6 -4 -2 0 2 4 6 8 10-4
-20
24
-2.0
-1.5
-1.0
-0.5
0.0
Pote
ntia
l
Y
X
( )12
L R−
( )12
L R+
Effect of proton-proton separation
2K
( )12
L R−
( )12
L R+
1sE K≅ −
1sE K≅ +
Effect of proton-proton separation
Atomic separation
4 8
Ene
rgy
Energy level separation as a function of lattice spacing
2K
bonding
antibonding
E1s
+ _
+
( )12
L R−
1sE K≅ +
( )12
L R+
1sE K≅ −
E1s
+ _ _
++
( )12
L R−
( )12
L R+
6
Es
( )12 L Rs s−
( )12 L Rs s+
Bonding and antibonding states built up from an s-orbital
Epx
( )12 x L xRp p+
( )12 xL xRp p−
Bonding and antibonding states built up from a px-orbital
Epz
( )12 zL zRp p−
( )12 zL zRp p+
Bonding and antibonding states built up from a pz-orbital
Homonuclear diatomic molecules
n εn (eV) l=0 l=1 l=2
n
.. …..
4 ε4= -0.85 4s 4p 4d
3 ε3= -1.51 3s 3p
3d
2 ε2= -3.40 2s 2p
1 ε1= -13.6 1s
O1s22s22p4
E2s
The O2 molecule
O O
2
-2
2
4-2E2p
7
The O2 molecule is magneticThe O2molecule is magnetic
E2s
E2p
n εn (eV) l=0 l=1 l=2
n
.. …..
4 ε4= -0.85 4s 4p 4d
3 ε3= -1.51 3s 3p
3d
2 ε2= -3.40 2s 2p
1 ε1= -13.6 1s
F1s22s22p5
The F2 molecule
2
-2
2
4-4
F F
E2p
E2s
n εn (eV) l=0 l=1 l=2
n
.. …..
4 ε4= -0.85 4s 4p 4d
3 ε3= -1.51 3s 3p
3d
2 ε2= -3.40 2s 2p
1 ε1= -13.6 1s
Ne1s22s22p6
The Ne2 molecule
Ne Ne
does not exist
2
-2
24
-4 -2
E2p
E2s
A little complication
8
n εn (eV) l=0 l=1 l=2
n
.. …..
4 ε4= -0.85 4s 4p 4d
3 ε3= -1.51 3s 3p
3d
2 ε2= -3.40 2s 2p
1 ε1= -13.6 1s
N1s22s22p3
Atomic radii (pm) The N2 molecule is not like this
E2p
The N2molecule is not
like this
E2s
2
-2
2
4
N N
The N2 molecule The N2molecule
N N E2s
E2p
2
-2
42
E2s
E2p E2pE2p
E2sE2s
The N2 molecule
right wrong
9
Heteronuclear diatomic molecules
Es
( )12 L Rs s−
( )12 L Rs s+
Homonuclear Heteronuclear
( )0.2 0.98L Rs s+
( )0.98 0.2L Rs s−
EL
ER
Polar bonding and antibonding states
( )0.2 0.98L Rs s+
( )0.98 0.2L Rs s−
EL
ER
E1sHydrogen
E2pFluor
H F
Ionic bond
H 1s
1s-13.6 eV
-0.7 eV
The electron affinity of H is
0.7 eV
F1s22s22p5
1s
2s 2p-18.6 eV
-3.3 eV
The electron affinity of F is
3.3 eV
10
F1s22s22p5H 1s
1s
2s 2p
1s-13.6 eV-18.6 eV
F1s22s22p5H 1s
1s
2s 2p
1s-13.6 eV-18.6 eV
-3.3 eV
The transfer of an electron from H to F costs 10.3 eV
F1s22s22p5H 1s
1s
2s 2p
1s-13.6 eV-18.6 eV
F1s22s22p5H 1s
1s
2s 2p
1s-13.6 eV-18.6 eV
The transfer of an electron from F to H costs 17.9 eV
-0.7 eV
1H
2He
3Li
4Be
5B
6C
7N
8O
9F
10Ne
11Na
12Mg
13Al
14Si
15P
16S
17Cl
18Ar
19K
20Ca
21Sc
22Ti
23V
24Cr
25Mn
26Fe
27Co
28Ni
29Cu
30Zn
31Ga
32Ge
33As
34Se
35Br
36Kr
37Rb
38Sr
39Y
40Zr
41Nb
42Mo
43Tc
44Ru
45Rh
46Pd
47Ag
48Cd
49In
50Sn
51Sb
52Te
53I
54Xe
55Cs
56Ba
57La
72Hf
73Ta
74W
75Re
76Os
77Ir
78Pt
79Au
80Hg
81Tl
82Pb
83Bi
84Po
85At
86Rn
87Fr
88Ra
89Ac57La
58Ce
59Pr
60Nd
61Pm
62Sm
63Eu
64Gd
65Tb
66Dy
67Ho
68Er
69Tm
70Yb
71Lu
1H
2He
3Li
4Be
5B
6C
7N
8O
9F
10Ne
11Na
12Mg
13Al
14Si
15P
16S
17Cl
18Ar
19K
20Ca
21Sc
22Ti
23V
24Cr
25Mn
26Fe
27Co
28Ni
29Cu
30Zn
31Ga
32Ge
33As
34Se
35Br
36Kr
37Rb
38Sr
39Y
40Zr
41Nb
42Mo
43Tc
44Ru
45Rh
46Pd
47Ag
48Cd
49In
50Sn
51Sb
52Te
53I
54Xe
55Cs
56Ba
57La
72Hf
73Ta
74W
75Re
76Os
77Ir
78Pt
79Au
80Hg
81Tl
82Pb
83Bi
84Po
85At
86Rn
87Fr
88Ra
89Ac57La
58Ce
59Pr
60Nd
61Pm
62Sm
63Eu
64Gd
65Tb
66Dy
67Ho
68Er
69Tm
70Yb
71Lu
11
http://www.webelements.com/webelements/scholar/properties/image-line/
1H
2He
3Li
4Be
5B
6C
7N
8O
9F
10Ne
11Na
12Mg
13Al
14Si
15P
16S
17Cl
18Ar
19K
20Ca
21Sc
22Ti
23V
24Cr
25Mn
26Fe
27Co
28Ni
29Cu
30Zn
31Ga
32Ge
33As
34Se
35Br
36Kr
37Rb
38Sr
39Y
40Zr
41Nb
42Mo
43Tc
44Ru
45Rh
46Pd
47Ag
48Cd
49In
50Sn
51Sb
52Te
53I
54Xe
55Cs
56Ba
57La
72Hf
73Ta
74W
75Re
76Os
77Ir
78Pt
79Au
80Hg
81Tl
82Pb
83Bi
84Po
85At
86Rn
87Fr
88Ra
89Ac57La
58Ce
59Pr
60Nd
61Pm
62Sm
63Eu
64Gd
65Tb
66Dy
67Ho
68Er
69Tm
70Yb
71Lu
http://www.webelements.com/webelements/scholar/properties/image-line/
1H
2He
3Li
4Be
5B
6C
7N
8O
9F
10Ne
11Na
12Mg
13Al
14Si
15P
16S
17Cl
18Ar
19K
20Ca
21Sc
22Ti
23V
24Cr
25Mn
26Fe
27Co
28Ni
29Cu
30Zn
31Ga
32Ge
33As
34Se
35Br
36Kr
37Rb
38Sr
39Y
40Zr
41Nb
42Mo
43Tc
44Ru
45Rh
46Pd
47Ag
48Cd
49In
50Sn
51Sb
52Te
53I
54Xe
55Cs
56Ba
57La
72Hf
73Ta
74W
75Re
76Os
77Ir
78Pt
79Au
80Hg
81Tl
82Pb
83Bi
84Po
85At
86Rn
87Fr
88Ra
89Ac57La
58Ce
59Pr
60Nd
61Pm
62Sm
63Eu
64Gd
65Tb
66Dy
67Ho
68Er
69Tm
70Yb
71Lu
2
,0
2
0
4
4
i ji j ij
d
e aE Q Qa r
eMa
πε
πε
=
= −
∑
For NaCl structure Md=1.7476
For CsCl structure Md=1.7627
Formation of an ionic solid
anearest neighbour distance
NaCl (ionic radii)
NaCl crystalas in the book
Ionic radii
12
NaCl with Na in an octahedral hole Ionic radii
CsCl with Cl in a cubic hole Ionic radii
CaF2 with F in a tetrahedral hole
jiji ij
QQraDE ∑=
,2
2
2
Formation of an ionic solid
Positive ion
Negative ion