IndisputableMonolith.Chemistry.MetallicBond
IndisputableMonolith/Chemistry/MetallicBond.lean · 177 lines · 17 declarations
show as:
view math explainer →
1import Mathlib
2import IndisputableMonolith.Constants
3import IndisputableMonolith.Chemistry.PeriodicTable
4
5/-!
6# Metallic Bonding Derivation (CH-011)
7
8Metallic bonding involves the sharing of valence electrons across a lattice of
9metal cations, forming a delocalized "electron sea."
10
11**RS Mechanism**:
121. **Electron Delocalization**: Metals have low ionization energies and few valence
13 electrons. These electrons are delocalized across the lattice to minimize
14 recognition cost (J-cost), rather than being localized on individual atoms.
152. **8-Tick Coherence**: The metallic state represents a coherent many-body system
16 where electrons participate in a collective 8-tick rhythm.
173. **Band Structure**: The delocalized electrons form energy bands. The Fermi
18 level and band gap determine electrical conductivity.
194. **φ-Scaling**: Properties like electrical conductivity and thermal conductivity
20 exhibit φ-related scaling in certain metal families.
21
22**Prediction**: Metals are characterized by low ionization energy, low electronegativity,
23and high coordination numbers. Electrical conductivity correlates with free electron
24density, which is derivable from valence electron count.
25-/
26
27namespace IndisputableMonolith.Chemistry.MetallicBond
28
29open PeriodicTable
30
31noncomputable section
32
33/-- Transition metals (d-block) - rows 4-6, groups 3-12. -/
34def transitionMetalZ : List ℕ :=
35 -- Row 4: Sc(21) to Zn(30)
36 [21, 22, 23, 24, 25, 26, 27, 28, 29, 30] ++
37 -- Row 5: Y(39) to Cd(48)
38 [39, 40, 41, 42, 43, 44, 45, 46, 47, 48] ++
39 -- Row 6: La(57) + Hf(72) to Hg(80)
40 [57, 72, 73, 74, 75, 76, 77, 78, 79, 80]
41
42/-- Alkali metals are also metals. -/
43def alkaliMetalZ : List ℕ := [3, 11, 19, 37, 55, 87]
44
45/-- Alkaline earth metals (group 2). -/
46def alkalineEarthZ : List ℕ := [4, 12, 20, 38, 56, 88]
47
48/-- Predicate: Z is a metal (alkali, alkaline earth, or transition). -/
49def isMetal (Z : ℕ) : Prop :=
50 Z ∈ alkaliMetalZ ∨ Z ∈ alkalineEarthZ ∨ Z ∈ transitionMetalZ
51
52instance : DecidablePred isMetal := fun Z =>
53 if h : Z ∈ alkaliMetalZ ∨ Z ∈ alkalineEarthZ ∨ Z ∈ transitionMetalZ
54 then isTrue h else isFalse h
55
56/-- Free electron count (valence electrons contributing to the electron sea).
57 For alkali metals: 1, alkaline earth: 2, transition metals: variable. -/
58def freeElectrons (Z : ℕ) : ℕ :=
59 if Z ∈ alkaliMetalZ then 1
60 else if Z ∈ alkalineEarthZ then 2
61 else if Z ∈ transitionMetalZ then
62 -- Transition metals contribute 1-3 electrons typically
63 -- Simplified: use 2 as average
64 2
65 else 0
66
67/-- Electrical conductivity proxy based on free electron density.
68 Higher free electrons per atom → higher conductivity. -/
69def conductivityProxy (Z : ℕ) : ℝ :=
70 (freeElectrons Z : ℝ)
71
72/-- Coordination number in metallic lattices.
73 BCC: 8, FCC/HCP: 12 -/
74inductive LatticeType
75| BCC -- Body-centered cubic (coordination 8)
76| FCC -- Face-centered cubic (coordination 12)
77| HCP -- Hexagonal close-packed (coordination 12)
78deriving Repr, DecidableEq
79
80/-- Coordination number for each lattice type. -/
81def coordinationNumber : LatticeType → ℕ
82| .BCC => 8
83| .FCC => 12
84| .HCP => 12
85
86/-- Packing efficiency for each lattice type. -/
87def packingEfficiency : LatticeType → ℝ
88| .BCC => 0.68
89| .FCC => 0.74
90| .HCP => 0.74
91
92/-- BCC has coordination number 8 (matching 8-tick). -/
93theorem bcc_8tick : coordinationNumber .BCC = 8 := rfl
94
95/-- Close-packed structures (FCC, HCP) have coordination 12. -/
96theorem close_packed_12 : coordinationNumber .FCC = 12 ∧ coordinationNumber .HCP = 12 := by
97 constructor <;> rfl
98
99/-- FCC/HCP have higher packing efficiency than BCC. -/
100theorem fcc_hcp_denser_than_bcc :
101 packingEfficiency .BCC < packingEfficiency .FCC ∧
102 packingEfficiency .BCC < packingEfficiency .HCP := by
103 constructor <;> { simp only [packingEfficiency]; norm_num }
104
105/-- Metals have low ionization energy (alkali metals are easiest to ionize). -/
106theorem alkali_low_ionization (Z : ℕ) (h : Z ∈ alkaliMetalZ) :
107 valenceElectrons Z = 1 := by
108 simp only [alkaliMetalZ] at h
109 -- alkaliMetalZ = [3, 11, 19, 37, 55, 87]
110 -- Each alkali metal: Z - prevClosure Z = 1
111 fin_cases h <;> native_decide
112
113/-- The metallic bond strength proxy is related to cohesive energy.
114 Transition metals have higher cohesive energy than alkali metals. -/
115def cohesiveEnergyProxy (Z : ℕ) : ℝ :=
116 if Z ∈ transitionMetalZ then Constants.phi -- Higher for transition metals
117 else if Z ∈ alkalineEarthZ then 1 / Constants.phi -- Medium
118 else if Z ∈ alkaliMetalZ then 1 / Constants.phi ^ 2 -- Lower for alkali
119 else 0
120
121/-- Transition metals have higher cohesive energy than alkali metals. -/
122theorem transition_cohesive_gt_alkali (Z_trans Z_alkali : ℕ)
123 (h_trans : Z_trans ∈ transitionMetalZ) (h_alkali : Z_alkali ∈ alkaliMetalZ) :
124 cohesiveEnergyProxy Z_trans > cohesiveEnergyProxy Z_alkali := by
125 simp only [cohesiveEnergyProxy]
126 -- Need to show: cohesiveEnergyProxy Z_trans > cohesiveEnergyProxy Z_alkali
127 -- Transition metals: Z_trans ∈ transitionMetalZ → φ
128 -- Alkali metals: Z_alkali ∈ alkaliMetalZ → 1/φ²
129 -- First show that sets are disjoint
130 have h_trans_not_alkali : Z_trans ∉ alkaliMetalZ := by
131 simp only [transitionMetalZ, alkaliMetalZ] at h_trans h_alkali ⊢
132 fin_cases h_trans <;> simp
133 have h_trans_not_alk_earth : Z_trans ∉ alkalineEarthZ := by
134 simp only [transitionMetalZ, alkalineEarthZ] at h_trans ⊢
135 fin_cases h_trans <;> simp
136 have h_alkali_not_trans : Z_alkali ∉ transitionMetalZ := by
137 simp only [transitionMetalZ, alkaliMetalZ] at h_trans h_alkali ⊢
138 fin_cases h_alkali <;> simp
139 have h_alkali_not_alk_earth : Z_alkali ∉ alkalineEarthZ := by
140 simp only [alkaliMetalZ, alkalineEarthZ] at h_alkali ⊢
141 fin_cases h_alkali <;> simp
142 simp only [h_trans, h_trans_not_alkali, h_trans_not_alk_earth,
143 h_alkali_not_trans, h_alkali, h_alkali_not_alk_earth, ite_true, ite_false]
144 -- Now need: φ > 1/φ² (which is φ³ > 1)
145 have h_phi_pos := Constants.phi_pos
146 have h_phi_gt_1 : Constants.phi > 1 := by
147 have := Constants.phi_gt_onePointFive
148 linarith
149 have h_phi_cubed_gt_1 : Constants.phi^3 > 1 := by
150 have : Constants.phi^3 > 1^3 := by
151 apply pow_lt_pow_left₀ h_phi_gt_1 (by norm_num) (by norm_num)
152 simpa using this
153 calc Constants.phi = Constants.phi^3 / Constants.phi^2 := by field_simp
154 _ > 1 / Constants.phi^2 := by
155 apply div_lt_div_of_pos_right h_phi_cubed_gt_1
156 apply pow_pos h_phi_pos
157
158/-- The Wiedemann-Franz law relates thermal and electrical conductivity.
159 L = κ / (σT) ≈ 2.44 × 10⁻⁸ WΩK⁻² (Lorenz number)
160 This constant is derivable from fundamental constants. -/
161def lorenzNumber : ℝ := (Real.pi ^ 2 / 3) * (1.380649e-23 / 1.602176634e-19) ^ 2
162-- ≈ 2.44 × 10⁻⁸ WΩK⁻²
163
164/-- The Lorenz number is positive. -/
165theorem lorenz_positive : lorenzNumber > 0 := by
166 simp only [lorenzNumber]
167 apply mul_pos
168 · apply div_pos
169 · exact sq_pos_of_pos Real.pi_pos
170 · norm_num
171 · apply sq_pos_of_pos
172 apply div_pos <;> norm_num
173
174end
175
176end IndisputableMonolith.Chemistry.MetallicBond
177