use super::polar::helmholtz_energy_density_polar;
use crate::hard_sphere::HardSphereProperties;
use crate::pcsaft::eos::dispersion::{A0, A1, A2, B0, B1, B2};
use crate::pcsaft::parameters::PcSaftPars;
use feos_core::FeosError;
use feos_dft::{FunctionalContribution, WeightFunction, WeightFunctionInfo, WeightFunctionShape};
use nalgebra::DVector;
use ndarray::*;
use num_dual::DualNum;
use std::f64::consts::{FRAC_PI_6, PI};
const PSI_DFT: f64 = 1.3862;
const PSI_PDGT: f64 = 1.3286;
#[derive(Clone)]
pub(crate) struct AttractiveFunctional<'a> {
parameters: &'a PcSaftPars,
}
impl<'a> AttractiveFunctional<'a> {
pub(crate) fn new(parameters: &'a PcSaftPars) -> Self {
Self { parameters }
}
}
fn att_weight_functions<N: DualNum<f64> + Copy>(
p: &PcSaftPars,
psi: f64,
temperature: N,
) -> WeightFunctionInfo<N> {
let d = p.hs_diameter(temperature);
let psi = N::from(psi);
WeightFunctionInfo::new(DVector::from_fn(d.len(), |i, _| i), false).add(
WeightFunction::new_scaled(d * psi, WeightFunctionShape::Theta),
false,
)
}
impl<'a> FunctionalContribution for AttractiveFunctional<'a> {
fn name(&self) -> &'static str {
"Attractive functional"
}
fn weight_functions<N: DualNum<f64> + Copy>(&self, temperature: N) -> WeightFunctionInfo<N> {
att_weight_functions(self.parameters, PSI_DFT, temperature)
}
fn weight_functions_pdgt<N: DualNum<f64> + Copy>(
&self,
temperature: N,
) -> WeightFunctionInfo<N> {
att_weight_functions(self.parameters, PSI_PDGT, temperature)
}
fn helmholtz_energy_density<N: DualNum<f64> + Copy>(
&self,
temperature: N,
density: ArrayView2<N>,
) -> Result<Array1<N>, FeosError> {
let p = &self.parameters;
let n = p.m.len();
let d = p.hs_diameter(temperature);
let d3m = d.zip_map(&p.m, |d, m| d.powi(3) * (m * FRAC_PI_6));
let eta = density.outer_iter().zip(&d3m).fold(
Array::zeros(density.raw_dim().remove_axis(Axis(0))),
|acc: Array1<N>, (rho, &d3m)| acc + &rho * d3m,
);
let mut rhog = Array::zeros(eta.raw_dim());
let mut m_bar = Array::zeros(eta.raw_dim());
for (rhoi, &mi) in density.axis_iter(Axis(0)).zip(p.m.iter()) {
m_bar += &(&rhoi * mi);
rhog += &rhoi;
}
m_bar.iter_mut().zip(rhog.iter()).for_each(|(m, &r)| {
if r.re() > f64::EPSILON {
*m /= r
} else {
*m = N::one()
}
});
let mut rho1mix: Array1<N> = Array::zeros(eta.raw_dim());
let mut rho2mix: Array1<N> = Array::zeros(eta.raw_dim());
for i in 0..n {
for j in 0..n {
let eps_ij_t = temperature.recip() * p.epsilon_k_ij[(i, j)];
let sigma_ij_3 = p.sigma_ij[(i, j)].powi(3);
rho1mix = rho1mix
+ (&density.index_axis(Axis(0), i) * &density.index_axis(Axis(0), j))
.mapv(|x| x * (eps_ij_t * sigma_ij_3 * p.m[i] * p.m[j]));
rho2mix = rho2mix
+ (&density.index_axis(Axis(0), i) * &density.index_axis(Axis(0), j))
.mapv(|x| x * (eps_ij_t * eps_ij_t * sigma_ij_3 * p.m[i] * p.m[j]));
}
}
let mut i1: Array1<N> = Array::zeros(eta.raw_dim());
let mut i2: Array1<N> = Array::zeros(eta.raw_dim());
let mut eta_i: Array1<N> = Array::ones(eta.raw_dim());
let m1 = (m_bar.clone() - 1.0) / &m_bar;
let m2 = (m_bar.clone() - 2.0) / &m_bar * &m1;
for i in 0..=6 {
i1 = i1 + (&m2 * A2[i] + &m1 * A1[i] + A0[i]) * &eta_i;
i2 = i2 + (&m2 * B2[i] + &m1 * B1[i] + B0[i]) * &eta_i;
eta_i = &eta_i * η
}
let c1 = Zip::from(&eta).and(&m_bar).map_collect(|&eta, &m| {
(m * (eta * 8.0 - eta.powi(2) * 2.0) / (eta - 1.0).powi(4)
+ (eta * (eta * (eta * (eta * 2.0 - 12.0) + 27.0) - 20.0))
/ ((eta - 1.0) * (eta - 2.0)).powi(2)
* (m - 1.0)
+ 1.0)
.recip()
});
let phi_polar = helmholtz_energy_density_polar(p, temperature, density)?;
Ok((-rho1mix * i1 * 2.0 - rho2mix * m_bar * c1 * i2) * PI + phi_polar)
}
}