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add ion_particle_flux and refactor NEO parsing #5

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55 changes: 22 additions & 33 deletions src/NEO.jl
Original file line number Diff line number Diff line change
Expand Up @@ -83,50 +83,39 @@ function run_neo(input_neo::InputNEO)
run(Cmd(`bash command.sh`; dir=folder))

### parse outputs ###
fluxes = Float64[]

tmp = open(joinpath(folder, "out.neo.transport_flux"), "r") do io
tmp_fluxes = Float64[]
open(joinpath(folder, "out.neo.transport_flux"), "r") do io
for line in eachline(io)
if !startswith(line, "#")
for word in split(line)
val = tryparse(Float64, word)
if val !== nothing
push!(fluxes, val)
push!(tmp_fluxes, val)
end
end
end
end
end

loc_first_tgyro = (4 * input_neo.N_SPECIES * 2) + 1
tgyro_fluxes = fluxes[loc_first_tgyro:end]

flux_solution = NEO.flux_solution()

for i in range(0, input_neo.N_SPECIES - 1)
species = i + 1
setfield!(flux_solution, Symbol("PARTICLE_FLUX_$species"), tgyro_fluxes[2+(i*4)])
setfield!(flux_solution, Symbol("ENERGY_FLUX_$species"), tgyro_fluxes[3+(i*4)])
setfield!(flux_solution, Symbol("MOMENTUM_FLUX_$species"), tgyro_fluxes[4+(i*4)])
end

energy_flux_electrons = getfield(flux_solution, Symbol("ENERGY_FLUX_$(input_neo.N_SPECIES)")) # electrons are always the last species in the list
total_ion_energy_flux = -energy_flux_electrons # exclude electron energy flux from total ion energy flux
particle_flux_electrons = getfield(flux_solution, Symbol("PARTICLE_FLUX_$(input_neo.N_SPECIES)"))

for field in fieldnames(NEO.flux_solution)
if ismissing(getfield(flux_solution, field))
setfield!(flux_solution, field, 0.0)
end

if occursin("ENERGY", string(field))
total_ion_energy_flux += getfield(flux_solution, field)
end
end

total_fluxes = IMAS.flux_solution(particle_flux_electrons, 0.0, energy_flux_electrons, total_ion_energy_flux)

return total_fluxes
tgyro_fluxes = tmp_fluxes[loc_first_tgyro:end]

# figure out indexes
e_index = [input_neo.N_SPECIES]
i_index = collect(1:input_neo.N_SPECIES-1)
particle_index(index) = 2 .+ ((index .- 1) .* 4)
energy_index(index) = 3 .+ ((index .- 1) .* 4)
momentum_index(index) = 4 .+ ((index .- 1) .* 4)

# sort fluxes
electrons_energy_flux = tgyro_fluxes[energy_index(e_index)]
electrons_particle_flux = tgyro_fluxes[particle_index(e_index)]
ion_particle_flux = tgyro_fluxes[particle_index(i_index)]
ion_total_energy_flux = sum(tgyro_fluxes[energy_index(i_index)])
ion_total_momentum_flux = sum(tgyro_fluxes[momentum_index(i_index)])

# assign fluxes to flux_solution structure
sol = IMAS.flux_solution(electrons_energy_flux, ion_total_energy_flux, electrons_particle_flux, ion_particle_flux, ion_total_momentum_flux)
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return sol
end

const document = Dict()
Expand Down
4 changes: 3 additions & 1 deletion src/chang_hinton.jl
Original file line number Diff line number Diff line change
Expand Up @@ -6,6 +6,7 @@
iion::Integer)

Calculates the neoclassical flux using Chang-Hinton model which has been modified assuming Zi = 1, and ni=ne

Ref: C.S. Chang, F.L. Hinton, Phys. Fluids 25, 1493–1494 (1982), https://doi.org/10.1063/1.863934
"""
function changhinton(
Expand Down Expand Up @@ -103,6 +104,7 @@ function changhinton(

qneo_gb = neo_rho_star_in^2

sol = IMAS.flux_solution(0.0, 0.0, 0.0, efluxi / qneo_gb)
# assign fluxes to flux_solution structure
sol = IMAS.flux_solution(0.0, efluxi / qneo_gb, 0.0, Float64[], 0.0)
return sol
end
11 changes: 6 additions & 5 deletions src/hirshman_sigmar.jl
Original file line number Diff line number Diff line change
Expand Up @@ -411,13 +411,14 @@ function HS_to_GB(HS_solution::Tuple{Vector{Float64},Vector{Float64}}, dd::IMAS.
pflux_norm = pflux_multi ./ Gamma_neo_GB
eflux_norm = eflux_multi ./ Q_neo_GB

particle_flux_e = pflux_norm[end]
energy_flux_e = eflux_norm[end]
energy_flux_i = sum(eflux_norm[1:end-1])
particle_flux_e = pflux_norm[end]
particle_flux_i = pflux_norm[1:end-1]

energy_flux_i = sum(eflux_norm) - energy_flux_e

HS_fluxes = IMAS.flux_solution(particle_flux_e, 0.0, energy_flux_e, energy_flux_i)
return HS_fluxes
# assign fluxes to flux_solution structure
sol = IMAS.flux_solution(energy_flux_e, energy_flux_i, particle_flux_e, particle_flux_i, 0.0)
return sol
end

"""
Expand Down
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