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in ui_check, tiling of seedx was leading to the first dimension being transformed into the second dimension, so this was fixed. Users can now set a new spin up option, where the spin-up loops over the total simulation time until total RO2 concentrations at the end of the simulation vary by less than 10%.
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/Users/user/Library/CloudStorage/OneDrive-TheUniversityofManchester/Man_Teach/research_experience/SAPHIR-STAR/PyCHAM_output/mcmAP_scheme/Baker_2024_Exp2p1 | ||
/Users/user/Documents/GitHub/PyCHAM/PyCHAM/output/mcmAP_scheme/20Nov_0900_0959_Base |
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res_file_name = /Users/user/Library/CloudStorage/OneDrive-TheUniversityofManchester/Man_Teach/research_experience/SAPHIR-STAR/PyCHAM_output/mcmAP_PRAMAP_scheme/Baker_2024_Exp2p1_zpc1e-4_it1e-3 | ||
chem_sch_name = mcmAP_PRAMAP_scheme.kpp | ||
xml_name = /Users/user/Library/CloudStorage/OneDrive-TheUniversityofManchester/Man_Teach/research_experience/SAPHIR-STAR/PyCHAM_input/MCM_PRAM_xml.xml | ||
total_model_time = 8.64e4 | ||
update_step = 3.6e2 | ||
recording_time_step = 3.6e3 | ||
temperature = 293.15 | ||
tempt = 0. | ||
p_init = 101325.0 | ||
rh = 0.52 | ||
rht = 0 | ||
# UVC lights on | ||
light_status = J_values.xlsx | ||
# note that the photon intensity for 254 nm in this file | ||
# has been tuned to give a photolysis rate of J(O1D) | ||
# i.e. O3 + hv = O1D of | ||
# 8x10-4 /s when the exposed light is at a minimum of 35 %, | ||
# which Baker et al. 2024 section 3.1 says is the minimum | ||
# J(O1D) rate. | ||
#act_flux_file = SAPHIR_STAR_UVC_Actinic_Flux_Spectrum.csv | ||
const_comp = H2O | ||
# initial concentrations of components (ppb) | ||
Comp0 = O3, CO, APINENE, OH | ||
C0 = 29., 0., 7.5, 3.4e-5 | ||
# continuously influxed components | ||
cont_infl = O3, APINENE, CO | ||
cont_infl_t = 0., 4.32e4 | ||
# based on Figure 2 of Baker et al. 2024, | ||
# we need to tune the Cinfl values so that | ||
# in both the with and without CO stages of | ||
# experiment O3 has a mixing ratio of 25 ppb, | ||
# alpha-pinene has a mixing ratio of 5 ppb and | ||
# CO has a mixing ratio of 0 ppm in the first | ||
# stage and a mixing ratio of 2.5 ppm | ||
# these give correct results for APINENE, O3 and CO | ||
# when light intensity | ||
# in photofile set to 2.3e14 photons/cm2/s, but | ||
# OH comes out around a factor of two higher than Figure 2 | ||
# observations | ||
# lights tuned down for O3 and OH agreement | ||
#Cinfl = 0.0076, 0.0089; 0.0028, 0.0028; 0., 0.69 | ||
# lights set to give same J(O1D) as in Baker paper | ||
#Cinfl = 0.0083, 0.011; 0.0033, 0.0033; 0., 0.67 | ||
Cinfl = 0.011, 0.016; 0.0033, 0.0033; 0., 0.67 | ||
# residence time of 63 minutes | ||
dil_fac = 0.000265 | ||
wall_on = 1 | ||
# gas-wall partitioning | ||
# 1.1e-2 /s for all species from Ehn et al. 2013, | ||
# from S3 of supplement of Baker et al. 2024: | ||
# 5.88e-3 /s for RO2, OH loss rate | ||
# (5 /s) is actually due to a 'background reactivity', so | ||
# it is stated in the chemical scheme | ||
# and HO2 wall loss rate of | ||
mass_trans_coeff = RO2_wall1_5.88e-3; HO2_wall1_2e-2 | ||
# once these components go to wall do not allow evaporation from wall | ||
vol_Comp = RO2_wall1, HO2_wall1 | ||
volP = 0., 0. | ||
eff_abs_wall_massC = 1.e0 | ||
chem_scheme_markers = {, RO2, +, C(ind_, ), , &, , , :, }, ;, | ||
# set the vapour pressure estimation method for HOMs | ||
HOMs_vp_method = Mohr2019 | ||
# only need to use the below variables for the seeded case | ||
number_size_bins = 1 | ||
pconc = 2.3e1 | ||
pconct = 0. | ||
pcont = 1 | ||
mean_rad = 3.0e-2 | ||
std = 1.5 | ||
Vwat_inc = 2 | ||
# 125 nm radius | ||
upper_part_size = 1.25e-1 | ||
z_prt_coeff = 1.e-4 | ||
int_tol = 1.e-3, 1.e-3 | ||
tracked_comp = O3, OH, HO2, APINENE | ||
pars_skip = 0 |
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Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,76 @@ | ||
res_file_name = /Users/user/Library/CloudStorage/OneDrive-TheUniversityofManchester/Man_Teach/research_experience/SAPHIR-STAR/PyCHAM_output/mcmAP_scheme/Baker_2024_Exp2p2_it1e-4 | ||
chem_sch_name = mcmAP_scheme.kpp | ||
xml_name = /Users/user/Library/CloudStorage/OneDrive-TheUniversityofManchester/Man_Teach/research_experience/SAPHIR-STAR/PyCHAM_input/MCM_PRAM_xml.xml | ||
total_model_time = 8.64e4 | ||
update_step = 3.6e2 | ||
recording_time_step = 3.6e3 | ||
temperature = 293.15 | ||
tempt = 0. | ||
p_init = 101325.0 | ||
rh = 0.52 | ||
rht = 0 | ||
# UVC lights on | ||
light_status = J_values.xlsx | ||
# note that the photon intensity for 254 nm in this file | ||
# has been tuned to give a photolysis rate of J(O1D) | ||
# i.e. O3 + hv = O1D of | ||
# 8x10-4 /s when the exposed light is at a minimum of 35 %, | ||
# which Baker et al. 2024 section 3.1 says is the minimum | ||
# J(O1D) rate. | ||
#act_flux_file = SAPHIR_STAR_UVC_Actinic_Flux_Spectrum.csv | ||
const_comp = H2O | ||
# initial concentrations of components (ppb) | ||
Comp0 = O3, CO, APINENE, OH | ||
C0 = 29., 0., 7.5, 3.4e-5 | ||
# continuously influxed components | ||
cont_infl = O3, APINENE, CO | ||
cont_infl_t = 0., 4.32e4 | ||
# based on Figure 2 of Baker et al. 2024, | ||
# we need to tune the Cinfl values so that | ||
# in both the with and without CO stages of | ||
# experiment O3 has a mixing ratio of 25 ppb, | ||
# alpha-pinene has a mixing ratio of 5 ppb and | ||
# CO has a mixing ratio of 0 ppm in the first | ||
# stage and a mixing ratio of 2.5 ppm | ||
# these give correct results for APINENE, O3 and CO | ||
# when light intensity | ||
# in photofile set to 2.3e14 photons/cm2/s, but | ||
# OH comes out around a factor of two higher than Figure 2 | ||
# observations | ||
# lights tuned down for O3 and OH agreement | ||
#Cinfl = 0.0076, 0.0089; 0.0028, 0.0028; 0., 0.69 | ||
# lights set to give same J(O1D) as in Baker paper | ||
#Cinfl = 0.0083, 0.011; 0.0033, 0.0033; 0., 0.67 | ||
Cinfl = 0.011, 0.015; 0.0033, 0.0033; 0., 0.67 | ||
# residence time of 63 minutes | ||
dil_fac = 0.000265 | ||
wall_on = 1 | ||
# gas-wall partitioning | ||
# 1.1e-2 /s for all species from Ehn et al. 2013, | ||
# from S3 of supplement of Baker et al. 2024: | ||
# 5.88e-3 /s for RO2, OH loss rate | ||
# (5 /s) is actually due to a 'background reactivity', so | ||
# it is stated in the chemical scheme | ||
# and HO2 wall loss rate of | ||
mass_trans_coeff = RO2_wall1_5.88e-3; HO2_wall1_2e-2 | ||
# once these components go to wall do not allow evaporation from wall | ||
vol_Comp = RO2_wall1, HO2_wall1 | ||
volP = 0., 0. | ||
eff_abs_wall_massC = 1.e0 | ||
chem_scheme_markers = {, RO2, +, C(ind_, ), , &, , , :, }, ;, | ||
# set the vapour pressure estimation method for HOMs | ||
HOMs_vp_method = Mohr2019 | ||
# only need to use the below variables for the seeded case | ||
number_size_bins = 0 | ||
#pconc = 1.8e1 | ||
#pconct = 0. | ||
#pcont = 1 | ||
#mean_rad = 3.0e-2 | ||
#std = 1.5 | ||
#Vwat_inc = 2 | ||
# 125 nm radius | ||
#upper_part_size = 1.25e-1 | ||
#z_prt_coeff = 1.e-4 | ||
int_tol = 1.e-4, 1.e-4 | ||
tracked_comp = O3, OH, HO2, APINENE | ||
pars_skip = 1 |
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