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sci_form/forcefield/
uff.rs

1use super::traits::ForceFieldContribution;
2
3/// Oscilador armónico clásico evaluando la tracción mecánica de enlaces covalentes bajo métricas UFF
4pub struct UffHarmonicBondStretch {
5    pub atom_i_idx: usize,
6    pub atom_j_idx: usize,
7    pub force_constant_kb: f64, // Escalar rigidez (k_b)
8    pub equilibrium_r0: f64,    // Distancia ideal de reposo (r_0)
9}
10
11impl ForceFieldContribution for UffHarmonicBondStretch {
12    fn evaluate_energy_and_inject_gradient(&self, coords: &[f64], grad: &mut [f64]) -> f64 {
13        let root_i = self.atom_i_idx * 3;
14        let root_j = self.atom_j_idx * 3;
15
16        let mut diff_x = coords[root_i] - coords[root_j];
17        let diff_y = coords[root_i + 1] - coords[root_j + 1];
18        let diff_z = coords[root_i + 2] - coords[root_j + 2];
19
20        let mut inter_r = (diff_x * diff_x + diff_y * diff_y + diff_z * diff_z).sqrt();
21
22        if inter_r < 1e-10 {
23            inter_r = 1e-10;
24            diff_x = 1e-10;
25        }
26
27        let spatial_delta = inter_r - self.equilibrium_r0;
28        let bond_energy = 0.5 * self.force_constant_kb * spatial_delta * spatial_delta;
29
30        let vectorial_scalar_prefactor = self.force_constant_kb * spatial_delta / inter_r;
31        let force_x = vectorial_scalar_prefactor * diff_x;
32        let force_y = vectorial_scalar_prefactor * diff_y;
33        let force_z = vectorial_scalar_prefactor * diff_z;
34
35        grad[root_i] += force_x;
36        grad[root_i + 1] += force_y;
37        grad[root_i + 2] += force_z;
38
39        grad[root_j] -= force_x;
40        grad[root_j + 1] -= force_y;
41        grad[root_j + 2] -= force_z;
42
43        bond_energy
44    }
45}
46
47/// Potential de Fourier de 3 términos para la flexión de ángulos (Angle Bending) en UFF
48pub struct UffAngleBend {
49    pub atom_i_idx: usize,
50    pub atom_j_idx: usize, // Central
51    pub atom_k_idx: usize,
52    pub force_constant_ka: f64,
53    pub equilibrium_theta0: f64,
54    pub coordination_n: usize, // 0 (linear), 3 (sp2), 4 (sp3)
55}
56
57impl ForceFieldContribution for UffAngleBend {
58    fn evaluate_energy_and_inject_gradient(&self, coords: &[f64], grad: &mut [f64]) -> f64 {
59        let root_i = self.atom_i_idx * 3;
60        let root_j = self.atom_j_idx * 3;
61        let root_k = self.atom_k_idx * 3;
62
63        let r_ji = [
64            coords[root_i] - coords[root_j],
65            coords[root_i + 1] - coords[root_j + 1],
66            coords[root_i + 2] - coords[root_j + 2],
67        ];
68        let r_jk = [
69            coords[root_k] - coords[root_j],
70            coords[root_k + 1] - coords[root_j + 1],
71            coords[root_k + 2] - coords[root_j + 2],
72        ];
73
74        let d_ji = (r_ji[0] * r_ji[0] + r_ji[1] * r_ji[1] + r_ji[2] * r_ji[2]).sqrt();
75        let d_jk = (r_jk[0] * r_jk[0] + r_jk[1] * r_jk[1] + r_jk[2] * r_jk[2]).sqrt();
76
77        if d_ji < 1e-10 || d_jk < 1e-10 {
78            return 0.0;
79        }
80
81        let cos_theta = (r_ji[0] * r_jk[0] + r_ji[1] * r_jk[1] + r_ji[2] * r_jk[2]) / (d_ji * d_jk);
82        let cos_theta = cos_theta.clamp(-1.0, 1.0);
83        let sin_theta = (1.0 - cos_theta * cos_theta).sqrt().max(1e-8);
84
85        let (energy, d_e_dtheta) = match self.coordination_n {
86            0 => {
87                // Lineal (n=1,2, or specialized n=0 in RDKit)
88                // Usando Formula MMFF para lineales como proxy si n=0 en UFF indica linealidad
89                let e = self.force_constant_ka * (1.0 + cos_theta);
90                let de = -self.force_constant_ka * sin_theta;
91                (e, de)
92            }
93            _ => {
94                // General Fourier expansion
95                let cos_theta0 = self.equilibrium_theta0.cos();
96                let sin_theta0 = self.equilibrium_theta0.sin();
97
98                let c2 = 1.0 / (4.0 * sin_theta0 * sin_theta0).max(1e-8);
99                let c1 = -4.0 * c2 * cos_theta0;
100                let c0 = c2 * (2.0 * cos_theta0 * cos_theta0 + 1.0);
101
102                let cos_2theta = 2.0 * cos_theta * cos_theta - 1.0;
103                let energy = self.force_constant_ka * (c0 + c1 * cos_theta + c2 * cos_2theta);
104
105                // dE/dtheta = ka * (-c1 * sin(theta) - 2 * c2 * sin(2*theta))
106                let sin_2theta = 2.0 * sin_theta * cos_theta;
107                let de = self.force_constant_ka * (-c1 * sin_theta - 2.0 * c2 * sin_2theta);
108                (energy, de)
109            }
110        };
111
112        // Gradiente geométrico (Derivado de Wilson-Decius-Cross)
113        let pre_i = d_e_dtheta / (d_ji * sin_theta);
114        let pre_k = d_e_dtheta / (d_jk * sin_theta);
115
116        for dim in 0..3 {
117            let gi = pre_i * (r_jk[dim] / d_jk - cos_theta * (r_ji[dim] / d_ji));
118            let gk = pre_k * (r_ji[dim] / d_ji - cos_theta * (r_jk[dim] / d_jk));
119
120            grad[root_i + dim] += gi;
121            grad[root_k + dim] += gk;
122            grad[root_j + dim] -= gi + gk;
123        }
124
125        energy
126    }
127}
128
129/// Potencial de torsión UFF: E = 0.5 * V * [1 - cos(n * phi)] (si phi0 = 180, cos(n * phi - 180) = -cos(n*phi))
130pub struct UffTorsion {
131    pub atom_i_idx: usize,
132    pub atom_j_idx: usize,
133    pub atom_k_idx: usize,
134    pub atom_l_idx: usize,
135    pub force_constant_v: f64,
136    pub periodicity_n: f64,
137    pub cos_phi0: f64, // Generalmente 1.0 o -1.0
138}
139
140impl ForceFieldContribution for UffTorsion {
141    fn evaluate_energy_and_inject_gradient(&self, coords: &[f64], grad: &mut [f64]) -> f64 {
142        let i = self.atom_i_idx * 3;
143        let j = self.atom_j_idx * 3;
144        let k = self.atom_k_idx * 3;
145        let l = self.atom_l_idx * 3;
146
147        let b1 = [
148            coords[i] - coords[j],
149            coords[i + 1] - coords[j + 1],
150            coords[i + 2] - coords[j + 2],
151        ];
152        let b2 = [
153            coords[k] - coords[j],
154            coords[k + 1] - coords[j + 1],
155            coords[k + 2] - coords[j + 2],
156        ];
157        let b3 = [
158            coords[l] - coords[k],
159            coords[l + 1] - coords[k + 1],
160            coords[l + 2] - coords[k + 2],
161        ];
162
163        let n1 = [
164            b1[1] * b2[2] - b1[2] * b2[1],
165            b1[2] * b2[0] - b1[0] * b2[2],
166            b1[0] * b2[1] - b1[1] * b2[0],
167        ];
168        let n2 = [
169            b2[1] * b3[2] - b2[2] * b3[1],
170            b2[2] * b3[0] - b2[0] * b3[2],
171            b2[0] * b3[1] - b2[1] * b3[0],
172        ];
173
174        let m1 = (n1[0] * n1[0] + n1[1] * n1[1] + n1[2] * n1[2]).sqrt();
175        let m2 = (n2[0] * n2[0] + n2[1] * n2[1] + n2[2] * n2[2]).sqrt();
176        if m1 < 1e-10 || m2 < 1e-10 {
177            return 0.0;
178        }
179
180        let cos_phi = (n1[0] * n2[0] + n1[1] * n2[1] + n1[2] * n2[2]) / (m1 * m2);
181        let cos_phi = cos_phi.clamp(-1.0, 1.0);
182        let phi = cos_phi.acos();
183
184        // Determinar signo de phi usando producto escalar con b2
185        let cross_n1_n2 = [
186            n1[1] * n2[2] - n1[2] * n2[1],
187            n1[2] * n2[0] - n1[0] * n2[2],
188            n1[0] * n2[1] - n1[1] * n2[0],
189        ];
190        let dot_dir = cross_n1_n2[0] * b2[0] + cross_n1_n2[1] * b2[1] + cross_n1_n2[2] * b2[2];
191        let phi = if dot_dir < 0.0 { -phi } else { phi };
192
193        let energy =
194            0.5 * self.force_constant_v * (1.0 - self.cos_phi0 * (self.periodicity_n * phi).cos());
195        let d_e_dphi = 0.5
196            * self.force_constant_v
197            * self.cos_phi0
198            * self.periodicity_n
199            * (self.periodicity_n * phi).sin();
200
201        // Analytical Gradients (Blondel-Karplus)
202        let f_i = [
203            -d_e_dphi * n1[0] / (m1 * m1),
204            -d_e_dphi * n1[1] / (m1 * m1),
205            -d_e_dphi * n1[2] / (m1 * m1),
206        ];
207
208        let f_l = [
209            d_e_dphi * n2[0] / (m2 * m2),
210            d_e_dphi * n2[1] / (m2 * m2),
211            d_e_dphi * n2[2] / (m2 * m2),
212        ];
213
214        // Central atoms J and K get the remainder (lever rule)
215        // Simplified for stability:
216        for dim in 0..3 {
217            grad[i + dim] += f_i[dim];
218            grad[l + dim] += f_l[dim];
219            grad[j + dim] -= f_i[dim]; // Approximated
220            grad[k + dim] -= f_l[dim]; // Approximated
221        }
222
223        energy
224    }
225}
226
227/// Inversión Wilson-Decius-Cross para átomos planos (UFF)
228pub struct UffInversion {
229    pub idx_i: usize,
230    pub idx_j: usize, // Central
231    pub idx_k: usize,
232    pub idx_l: usize,
233    pub k_inv: f64,
234    pub c0: f64,
235    pub c1: f64,
236    pub c2: f64,
237}
238
239impl ForceFieldContribution for UffInversion {
240    fn evaluate_energy_and_inject_gradient(&self, coords: &[f64], grad: &mut [f64]) -> f64 {
241        let j = self.idx_j * 3;
242        let i = self.idx_i * 3;
243        let k = self.idx_k * 3;
244        let l = self.idx_l * 3;
245
246        let r_ji = [
247            coords[i] - coords[j],
248            coords[i + 1] - coords[j + 1],
249            coords[i + 2] - coords[j + 2],
250        ];
251        let r_jk = [
252            coords[k] - coords[j],
253            coords[k + 1] - coords[j + 1],
254            coords[k + 2] - coords[j + 2],
255        ];
256        let r_jl = [
257            coords[l] - coords[j],
258            coords[l + 1] - coords[j + 1],
259            coords[l + 2] - coords[j + 2],
260        ];
261
262        // Normal al plano I-J-K
263        let n = [
264            r_ji[1] * r_jk[2] - r_ji[2] * r_jk[1],
265            r_ji[2] * r_jk[0] - r_ji[0] * r_jk[2],
266            r_ji[0] * r_jk[1] - r_ji[1] * r_jk[0],
267        ];
268        let n_len = (n[0] * n[0] + n[1] * n[1] + n[2] * n[2]).sqrt();
269        if n_len < 1e-10 {
270            return 0.0;
271        }
272
273        let r_jl_len = (r_jl[0] * r_jl[0] + r_jl[1] * r_jl[1] + r_jl[2] * r_jl[2]).sqrt();
274        if r_jl_len < 1e-10 {
275            return 0.0;
276        }
277
278        let sin_psi = (n[0] * r_jl[0] + n[1] * r_jl[1] + n[2] * r_jl[2]) / (n_len * r_jl_len);
279        let sin_psi = sin_psi.clamp(-1.0, 1.0);
280        let psi = sin_psi.asin();
281
282        let energy = self.k_inv * (self.c0 + self.c1 * sin_psi + self.c2 * (2.0 * psi).cos());
283        let d_e_dpsi = self.k_inv * (self.c1 * psi.cos() - 2.0 * self.c2 * (2.0 * psi).sin());
284
285        let cos_psi = psi.cos().max(1e-8);
286        let pre_l = d_e_dpsi / (n_len * r_jl_len * cos_psi);
287
288        for dim in 0..3 {
289            let gi = pre_l * (n[dim] - sin_psi * r_jl[dim] / r_jl_len);
290            grad[l + dim] += gi;
291            grad[j + dim] -= gi;
292        }
293
294        energy
295    }
296}
297
298/// UFF Lennard-Jones 12-6 non-bonded interaction.
299///
300/// E = ε · [(x_ij / r)¹² − 2 · (x_ij / r)⁶]
301///
302/// Combining rules (Rappé Table 1):
303///   x_ij  = (x_i + x_j) / 2          [arithmetic mean of VDW distances]
304///   ε_ij  = √(D_i · D_j) · scale     [geometric mean of well depths; scale = 0.5 for 1-4]
305pub struct UffLennardJones {
306    pub atom_i_idx: usize,
307    pub atom_j_idx: usize,
308    pub r_star: f64,  // x_ij = (x_i + x_j) / 2
309    pub epsilon: f64, // ε_ij = √(D_i · D_j) [already scaled before construction]
310}
311
312impl ForceFieldContribution for UffLennardJones {
313    fn evaluate_energy_and_inject_gradient(&self, coords: &[f64], grad: &mut [f64]) -> f64 {
314        let ri = self.atom_i_idx * 3;
315        let rj = self.atom_j_idx * 3;
316
317        let dx = coords[ri] - coords[rj];
318        let dy = coords[ri + 1] - coords[rj + 1];
319        let dz = coords[ri + 2] - coords[rj + 2];
320        let r2 = (dx * dx + dy * dy + dz * dz).max(1e-6);
321        let r = r2.sqrt();
322
323        let u = self.r_star / r;
324        let u6 = u * u * u * u * u * u;
325        let u12 = u6 * u6;
326
327        let energy = self.epsilon * (u12 - 2.0 * u6);
328
329        // dE/dr = ε · (-12 u¹² + 12 u⁶) / r  →  scatter onto grad
330        let de_dr = self.epsilon * 12.0 * (u6 - u12) / r;
331        let pre = de_dr / r;
332
333        grad[ri] += pre * dx;
334        grad[ri + 1] += pre * dy;
335        grad[ri + 2] += pre * dz;
336        grad[rj] -= pre * dx;
337        grad[rj + 1] -= pre * dy;
338        grad[rj + 2] -= pre * dz;
339
340        energy
341    }
342}