From 3003655025909fb234f5c739c41df09952999c36 Mon Sep 17 00:00:00 2001 From: "Thomas A. Christensen II" <25492070+MillironX@users.noreply.github.com> Date: Tue, 3 Mar 2020 09:49:02 -0800 Subject: [PATCH] Add previously written UNIFAC method --- src/UNIFAC.jl | 197 +++++++++++++++++++++++++++++++++++++++++++++++++- 1 file changed, 196 insertions(+), 1 deletion(-) diff --git a/src/UNIFAC.jl b/src/UNIFAC.jl index c2cce4b..0635892 100644 --- a/src/UNIFAC.jl +++ b/src/UNIFAC.jl @@ -1,5 +1,200 @@ +# Thomas A. Christensen II +# Spring 2020 +# UNIFAC Solver + module UNIFAC -greet() = print("Hello World!") +export unifac + +function unifac(ν, x, T) +# unifac takes three arguments: +# ν (that's the Greek lowercase nu) is a 42 x n Integer array where n is the +# number of species in the system. The number at ν[k,i] indicates how many +# instances of subgroup k are present in a single molecule of species i +# x is a 1 x n Float64 array that contains the liquid species mole fractions +# T is the temperature of the system in Kelvins + + # Declare the UNIFAC subgroup parameters + R = Array{Float64}(undef, 42, 1) + R[1] = 0.9011 + R[2] = 0.6744 + R[3] = 0.4469 + R[4] = 0.2195 + R[10] = 0.5313 + R[12] = 1.2663 + R[13] = 1.0396 + R[15] = 1.0000 + R[17] = 0.9200 + R[19] = 1.6724 + R[20] = 1.4457 + R[25] = 1.1450 + R[26] = 0.9183 + R[27] = 0.6908 + R[32] = 1.4337 + R[33] = 1.2070 + R[34] = 0.9795 + R[41] = 1.8701 + R[42] = 1.6434 + + Q = Array{Float64}(undef, 42, 1) + Q[1] = 0.848 + Q[2] = 0.540 + Q[3] = 0.228 + Q[4] = 0.000 + Q[10] = 0.400 + Q[12] = 0.968 + Q[13] = 0.660 + Q[15] = 1.200 + Q[17] = 1.400 + Q[19] = 1.488 + Q[20] = 1.180 + Q[25] = 1.088 + Q[26] = 0.780 + Q[27] = 0.468 + Q[32] = 1.244 + Q[33] = 0.936 + Q[34] = 0.624 + Q[41] = 1.724 + Q[42] = 1.416 + + # Declare the subgroup interaction parameters + a = zeros(42, 42) + a[1:4, 10] .= 61.13 + a[1:4, 12:13] .= 76.50 + a[1:4, 15] .= 986.50 + a[1:4, 17] .= 1318.00 + a[1:4, 19:20] .= 476.40 + a[1:4, 25:27] .= 251.50 + a[1:4, 32:34] .= 255.70 + a[1:4, 41:42] .= 597.00 + + a[10, 1:4] .= -11.12 + a[10, 12:13] .= 167.00 + a[10, 15] = 636.10 + a[10, 17] = 903.80 + a[10, 19:20] .= 25.77 + a[10, 25:27] .= 32.14 + a[10, 32:34] .= 122.80 + a[10, 41:42] .= 212.50 + + a[12:13, 1:4] .= -69.70 + a[12:13, 10] .= -146.80 + a[12:13, 15] .= 803.20 + a[12:13, 17] .= 5695.00 + a[12:13, 19:20] .= -52.10 + a[12:13, 25:27] .= 213.10 + a[12:13, 32:34] .= -49.29 + a[12:13, 41:42] .= 6096.00 + + a[15, 1:4] .= 156.40 + a[15, 10] = 89.60 + a[15, 12:13] .= 25.82 + a[15, 17] = 353.50 + a[15, 19:20] .= 84.00 + a[15, 25:27] .= 28.06 + a[15, 32:34] .= 42.70 + a[15, 41:42] .= 6.712 + + a[17, 1:4] .= 300.00 + a[17, 10] = 362.30 + a[17, 12:13] .= 377.60 + a[17, 15] = -229.10 + a[17, 19:20] .= -195.40 + a[17, 25:27] .= 540.50 + a[17, 32:34] .= 168.00 + a[17, 41:42] .= 112.60 + + a[19:20, 1:4] .= 26.79 + a[19:20, 10] .= 140.10 + a[19:20, 12:13] .= 365.80 + a[19:20, 15] .= 164.50 + a[19:20, 17] .= 472.50 + a[19:20, 25:27] .= -103.60 + a[19:20, 32:34] .= -174.20 + a[19:20, 41:42] .= 481.70 + + a[25:27, 1:4] .= 83.36 + a[25:27, 10] .= 52.13 + a[25:27, 12:13] .= 65.69 + a[25:27, 15] .= 237.70 + a[25:27, 17] .= -314.70 + a[25:27, 19:20] .= 191.10 + a[25:27, 32:34] .= 251.50 + a[25:27, 41:42] .= -18.51 + + a[32:34, 1:4] .= 65.33 + a[32:34, 10] .= -22.31 + a[32:34, 12:13] .= 223.00 + a[32:34, 15] .= -150.00 + a[32:34, 17] .= -448.20 + a[32:34, 19:20] .= 394.60 + a[32:34, 25:27] .= -56.08 + a[32:34, 41:42] .= 147.10 + + a[41:42, 1:4] .= 24.82 + a[41:42, 10] .= -22.97 + a[41:42, 12:13] .= -138.40 + a[41:42, 15] .= 185.40 + a[41:42, 17] .= 242.80 + a[41:42, 19:20] .= -287.50 + a[41:42, 25:27] .= 38.81 + a[41:42, 32:34] .= -108.50 + + # Calculate r + r = zeros(1, size(ν, 2)) + for i in 1:size(ν, 2) + r[i] = sum(ν[:, i] .* R) + end + + # Calculate q + q = zeros(1, size(ν, 2)) + for i in 1:size(ν, 2) + q[i] = sum(ν[:, i] .* Q) + end + + # Calculate e + e = zeros(42, size(ν, 2)) + for i in 1:size(ν,2 ) + e[:, i] = (ν[:, i] .* Q) ./ q[i] + end + + # Calculate tau + τ = exp.(-a ./ T) + + # Calculate beta + β = zeros(42, size(ν, 2)) + for i in 1:size(ν, 2) + for k in 1:42 + β[k, i] = sum(e[:, i] .* τ[:, k]) + end + end + + # Calculate Theta + Θ = zeros(42, 1) + for k in 1:42 + Θ[k] = sum(x .* q .* e[k, :]') / sum(x .* q) + end + + # Calculate s + s = zeros(42, 1) + for k in 1:42 + s[k] = sum(Θ .* τ[:, k]) + end + + # Calculate L and J + L = r ./ sum(r .* x) + J = q ./ sum(q .* x) + + # Calculate the natural log of the cumulative and residual activity coefficients + γ_C = 1 .- J .+ log.(J) .- 5 .* q .* (1 .- (J ./ L) .+ log.(J ./ L)) + γ_R = zeros(1, size(ν, 2)) + for i in 1:size(ν, 2) + γ_R[i] = q[i] * (1 - sum(Θ .* β[:, i] ./ s .- e[:, i] .* log.(β[:, i] ./ s))) + end + + # Return the activity coefficients + γ = exp.(γ_C .+ γ_R) + +end # function end # module