| Flag name | Default value | Description |
| bmr_enhance_basal_water_pressure | "no" | if 'yes' then add basal melt rate enhancement to determination of basal water pressure, which normally only depends on effective thickness of basal water (=bwat) |
| compute_surf_grad_inward_ssa | "no" | [missing] |
| correct_cell_areas | "yes" | Compute corrected cell areas using WGS84 datum (for ice area and volume computations). |
| do_age | "no" | Solve age equation (advection equation for ice age). |
| do_cold_ice_methods | "no" | Use cold ice (i.e. not polythermal) methods. |
| do_mass_conserve | "yes" | Solve the mass conservation equation |
| do_pseudo_plastic_till | "no" | Use the pseudo-plastic till model. |
| do_skip | "no" | Use the temperature, age, and SSA stress balance computation skipping mechanism. |
| do_superpose | "yes" | Combine the velocity fields from the SIA and SSA models as in [BBssasliding]. Only effective if used with -ssa_sliding. |
| do_temp | "yes" | Solve energy conservation equations. |
| floating_ice_killed | "false" | If ice is (or becomes) floating then it is set to thickness zero. This is calving at the grounding line. |
| force_full_diagnostics | "no" | Force full diagnostic output (adds 3D velocity fields and velocity components at the surface |
| force_output_times | "yes" | Modify the time-stepping mechanism to hit times requested using -extra_times and -ts_times. |
| include_bmr_in_continuity | "yes" | Include basal melt rate in the continuity equation |
| is_dry_simulation | "no" | Dry (oceanless) simulation |
| ocean_kill | "false" | If used with input from a NetCDF initialization file which has ice-free ocean mask (value MASK_FLOATING_OCEAN0=7), will zero out ice thicknesses in areas that were ice-free ocean at time zero. This is calving at the location of the original calving front. |
| pdd_limit_timestep | "false" | Limit PDD time-step to 1 year; used by pclimate to make long runs faster. Is not and should not be used elsewhere. |
| thermal_bedrock | "yes" | Use the bedrock thermal model |
| thk_eff_basal_water_pressure | "no" | if 'yes' then modeled basal water pressure experiences decreases at locations where thickness is smaller than thk_eff_H_high (typically near margin; thickness is surrogate for distance to margin) |
| use_constant_nuh_for_ssa | "no" | Compute velocities in ice shelves and streams with a constant value for the product of viscosity and thickness , obtained from the shelf extension |
| use_eta_transformation | "yes" | Use eta transformation to compute surface gradient. |
| use_ssa_velocity | "no" | Use the equations of the shallow shelf approximation [MacAyeal, Morland, SchoofStream, WeisGreveHutter] for ice shelves and dragging ice shelves (i.e. ice streams) where so-indicated by the mask |
| use_ssa_when_grounded | "no" | In PISM, sliding occurs at all grounded points either in the SIA paradigm (see mu_sliding) or in the SSA-as-a-sliding law paradigm [BBssasliding]. Choose the latter if yes. |
| Parameter name | Default value | Description |
| Glen_exponent | 3 | ; Glen exponent in ice flow law |
| Hooke_A | 4.421650e-09 | s-1 Pa-3; A_Hooke = (1/B_0)^n where n=3 and B_0 = 1.928 a^(1/3) Pa. See [Hooke] |
| Hooke_C | 0.166120 | Kelvin^Hooke_k; See [Hooke] |
| Hooke_Q | 78800 | J / mol; Activation energy, see [Hooke] |
| Hooke_Tr | 273.390000 | Kelvin; See [Hooke] |
| Hooke_k | 1.170000 | ; See [Hooke] |
| Paterson-Budd_A_cold | 3.610000e-13 | Pa^-3 / s; Paterson-Budd A_cold, see [PatersonBudd] |
| Paterson-Budd_A_warm | 1730 | Pa^-3 / s; Paterson-Budd A_warm, see [PatersonBudd] |
| Paterson-Budd_Q_cold | 60000 | J/mol; Paterson-Budd Q_cold, see [PatersonBudd] |
| Paterson-Budd_Q_warm | 139000 | J/mol; Paterson-Budd Q_warm, see [PatersonBudd] |
| Paterson-Budd_critical_temperature | 263.150000 | Kelvin; Paterson-Budd critical temperature, see [PatersonBudd] |
| Schoof_regularizing_length | 1000 | km; Regularizing length (Schoof definition) |
| Schoof_regularizing_velocity | 1 | m/year; Regularizing velocity (Schoof definition) |
| WGS84_semimajor_axis | 6378137 | m; WGS84 reference ellipsoid semi-major axis |
| WGS84_semiminor_axis | 6356752.314245 | m; WGS84 reference ellipsoid semi-minor axis |
| adaptive_timestepping_ratio | 0.120000 | ; Adaptive time stepping ratio for the explicit scheme for the mass balance equation; BBL, inequality (25) |
| bed_def_interval_years | 10 | years; Interval between bed deformation updates |
| bedrock_thermal_conductivity | 3 | J m-1 K-1 s-1; = W m-1 K-1; for bedrock used in thermal model [RitzEISMINT] |
| bedrock_thermal_density | 3300 | kg m-3; for bedrock used in thermal model |
| bedrock_thermal_specific_heat_capacity | 1000 | J kg-1 K-1; for bedrock used in thermal model [RitzEISMINT] |
| beta_CC | 7.900000e-08 | K Pa-1; Clausius-Clapeyron constant [Luethi2002] |
| beta_shelves_drag_too | 180000 | Pa s m^{-1}; (1/10000) of value stated in [HulbeMacAyeal] for ice stream E |
| bmr_enhance_scale | 3.168876e-09 | m s-1; = 0.10 m a-1; level at which basal melt rate starts making major difference in water pressure |
| bootstrapping_H_value_no_var | 0 | m; thickness value to use if thk (land_ice_thickness) variable is absent in bootstrapping file |
| bootstrapping_Hmelt_value_no_var | 0 | m; basal melt water effective thickness value to use if variable Hmelt is absent in bootstrapping file |
| bootstrapping_bed_value_no_var | 1 | m; bed elevation value to use if topg (bedrock_altitude) variable is absent in bootstrapping file |
| bootstrapping_bmelt_value_no_var | 0 | m s-1; basal melt rate value to use if variable bmelt is absent in bootstrapping file |
| bootstrapping_geothermal_flux_value_no_var | 0.042000 | W m-2; geothermal flux value to use if bheatflx variable is absent in bootstrapping file |
| bootstrapping_tillphi_value_no_var | 15 | degrees; till friction angle value to use if variable tillphi is absent in bootstrapping file; tends not to slip |
| bootstrapping_uplift_value_no_var | 0 | m s-1; uplift value to use if dbdt variable is absent in bootstrapping file |
| climate_forcing_buffer_size | 60 | ; number of 2D climate forcing records to keep in memory; = 5 years of monthly records |
| cold_base_refreeze_rate | 6.337753e-10 | m s-1; = 2 cm/yr; in enthalpy model, if base of ice is colder than pressure-melting, but there is positive-thickness stored basal water, then ice is added back at this rate |
| constant_grain_size | 1 | mm; Default constant grains size to use with the Goldsby-Kohlstedt [GoldsbyKohlstedt] flow law |
| default_tauc | 10000 | Pa; fill value for yield stress for basal till (plastic or pseudo-plastic model); note 10^4 Pa = 0.1 bar |
| default_till_phi | 30 | degrees; fill value for till friction angle |
| enhancement_factor | 1 | ; Flow enhancement factor |
| enthalpy_temperate_diffusivity | 0 | m2 s-1; diffusivity units same as k/(rho c) |
| epsilon_ssa | 1.000000e+15 | initial amount of (denominator) regularization in computation of effective viscosity |
| force_to_thickness_alpha | 6.337753e-11 | s-1; = 0.002 a-1; exponential coefficient in force-to-thickness mechanism |
| fresh_water_density | 1000 | kg m-3; |
| global_min_allowed_temp | 200 | Kelvin; Minimum allowed ice temperature |
| gpbld_water_frac_coeff | 184 | ; coefficient in Glen-Paterson-Budd flow law for extra dependence of softness on liquid water fraction (omega) [AschwandenBlatter, LliboutryDuval1985] |
| grid_Lbz | 0 | meters; Thickness of the thermal bedrock layer. |
| grid_Lx | 1500000 | m; Default computational box is 3000 km x 3000 km (= 2 Lx x 2 Ly) in horizontal. |
| grid_Ly | 1500000 | m; Default computational box is 3000 km x 3000 km (= 2 Lx x 2 Ly) in horizontal. |
| grid_Lz | 4000 | meters; Height of the computational domain. |
| grid_Mbz | 1 | ; Number of thermal bedrock layers; 1 level corresponds to no bedrock. |
| grid_Mx | 61 | ; Number of grid points in the x direction. |
| grid_My | 61 | ; Number of grid points in the y direction. |
| grid_Mz | 31 | ; Number of vertical grid levels in the ice. |
| grid_lambda | 4 | ; Vertical grid spacing parameter. Roughly equal to the factor by which the grid is coarser at an end away from the ice-bedrock interface. |
| hmelt_diffusion_distance | 20000 | meters; diffusion distance for melt water thickness; see equation (11) in [BBssasliding] |
| hmelt_diffusion_time | 1000 | years; diffusion time for melt water thickness; see equation (11) in [BBssasliding] |
| hmelt_max | 2 | meters; maximum thickness of the basal melt water layer |
| ice_density | 910 | kg m-3; = rho_i; density of ice in ice sheet |
| ice_softness | 4.000000e-25 | Pa-3 s-1; ice softness |
| ice_specific_heat_capacity | 2009 | J kg-1 K-1; at triple point T_0 |
| ice_thermal_conductivity | 2.100000 | J m-1 K-1 s-1; = W m-1 K-1 |
| ideal_gas_constant | 8.314410 | J mol-1 K-1; ideal gas constant |
| initial_age_of_ice_years | 0 | years; Initial age of ice |
| liquid_water_fraction_max | 0.010000 | pure number; in enthalpy model, drain once omega reaches this value [Greve97Greenland] |
| lithosphere_density | 3300 | kg m-3; lithosphere density used by the bed deformation model. See [LingleClark, BLKfastearth] |
| lithosphere_flexural_rigidity | 5.000000e+24 | N m; lithosphere flexural rigidity used by the bed deformation model. See [LingleClark, BLKfastearth] |
| mantle_viscosity | 1.000000e+21 | Pa s; half-space (mantle) viscosity used by the bed deformation model. See [LingleClark, BLKfastearth] |
| max_iterations_ssa | 300 | Maximum number of iterations for the ice viscosity computation |
| max_low_temp_count | 10 | Maximum number of grid points with ice temperature below global_min_allowed_temp. |
| maximum_time_step_years | 60 | years; Maximum allowed time step length |
| minimum_temperature_for_sliding | 273 | Kelvin; Note less than ice.meltingTemp; if above this value then decide to slide |
| mu_sliding | 0 | The sliding law parameter in SIA sliding paradigm. This kind of sliding is not recommended, which is why it is turned off by default. See Appendix B of BBssasliding for the dangers in this mechanism. |
| ocean_sub_shelf_heat_flux_into_ice | 0.500000 | W m-2; = J m-2 s-1; naively chosen default value for heat from ocean; see comments in src/coupler/PISMOcean.cc |
| pdd_factor_ice | 0.008000 | m K-1 day-1; EISMINT-Greenland value [RitzEISMINT] ; = (8 mm ice-equivalent) / (pos degree day) |
| pdd_factor_snow | 0.003000 | m K-1 day-1; EISMINT-Greenland value [RitzEISMINT] ; = (3 mm ice-equivalent) / (pos degree day) |
| pdd_fausto_T_c | 272.150000 | Kelvin; = -1 + 273.15; for formula (6) in [Faustoetal2009] |
| pdd_fausto_T_w | 283.150000 | Kelvin; = 10 + 273.15; for formula (6) in [Faustoetal2009] |
| pdd_fausto_beta_ice_c | 0.015000 | m day-1 K-1; water-equivalent thickness; for formula (6) in [Faustoetal2009] |
| pdd_fausto_beta_ice_w | 0.007000 | m day-1 K-1; water-equivalent thickness; for formula (6) in [Faustoetal2009] |
| pdd_fausto_beta_snow_c | 0.003000 | m day-1 K-1; water-equivalent thickness; for formula (6) in [Faustoetal2009] |
| pdd_fausto_beta_snow_w | 0.003000 | m day-1 K-1; water-equivalent thickness; for formula (6) in [Faustoetal2009] |
| pdd_fausto_latitude_beta_w | 72 | degrees N; latitude below which to use warm case, in formula (6) in [Faustoetal2009] |
| pdd_refreeze | 0.600000 | pure fraction; EISMINT-Greenland value [RitzEISMINT] |
| pdd_std_dev | 2.530000 | Kelvin; std dev of daily temp variation; value from [Faustoetal2009]; compare EISMINT-Greenland value of 5.0 [RitzEISMINT] |
| plastic_regularization | 0.010000 | Set the value of regularization of plastic till; this is the second in formula (4.1) in [SchoofStream] |
| precip_exponential_factor_for_temperature | 0.070417 | Kelvin-1; = 0.169/2.4; in SeaRISE-Greenland formula for paleo-precipitation from present; a 7.3% change of precipitation rate for every one degC of temperature change [Huybrechts02] |
| pseudo_plastic_q | 0.250000 | ; The exponent of the pseudo-plastic basal resistance model |
| pseudo_plastic_uthreshold | 100 | m a-1; |
| run_length_years | 1000 | years; Default run length |
| sea_water_density | 1028 | kg m-3; |
| seconds_per_year | 3.155693e+07 | ; should match the one used by UDUNITS (see src/udunits/pismudunits.dat). |
| skip_max | 10 | Number of mass-balance steps, including SIA diffusivity updates, to perform before a the temperature, age, and SSA stress balance computations are done |
| slice_level | 0 | meters; level (in meters above the base of ice) used in slice viewers |
| snow_temp_fausto_c_ma | -0.718900 | Kelvin (degN)-1; latitude-dependence coefficient for formula (1) in [Faustoetal2009] |
| snow_temp_fausto_c_mj | -0.158500 | Kelvin (degN)-1; latitude-dependence coefficient for formula (2) in [Faustoetal2009] |
| snow_temp_fausto_d_ma | 314.980000 | K; = 41.83+273.15; base temperature for formula (1) in [Faustoetal2009] |
| snow_temp_fausto_d_mj | 287.850000 | Kelvin; = 14.70+273.15; base temperature for formula (2) in [Faustoetal2009] |
| snow_temp_fausto_gamma_ma | -0.006309 | Kelvin m-1; = -6.309 / 1km; mean slope lapse rate for formula (1) in [Faustoetal2009] |
| snow_temp_fausto_gamma_mj | -0.005426 | Kelvin m-1; = -5.426 / 1km; mean slope lapse rate for formula (2) in [Faustoetal2009] |
| snow_temp_fausto_kappa_ma | 0.067200 | Kelvin (degW)-1; longitude-dependence coefficient for formula (1) in [Faustoetal2009] |
| snow_temp_fausto_kappa_mj | 0.051800 | Kelvin (degW)-1; longitude-dependence coefficient for formula (2) in [Faustoetal2009] |
| snow_temp_july_day | 196 | day; = Julian day for July 15; used in corrected formula (4) in [Faustoetal2009] |
| ssa_relative_convergence | 0.000100 | Relative change tolerance for the effective viscosity |
| standard_gravity | 9.810000 | m s-2; acceleration due to gravity on Earth geoid |
| start_year | 0 | years; Start year. |
| summary_volarea_scale_factor_log10 | 6 | ; an integer; log base 10 of scale factor to use for volume and area in summary line to stdout |
| surface_pressure | 0 | Pa; atmospheric pressure; = pressure at ice surface |
| thk_eff_H_high | 2000 | m; maximum thickness at which thickness effect on basal water pressure is applied |
| thk_eff_H_low | 1000 | m; thickness at which thickness effect on basal water pressure is full strength |
| thk_eff_reduced | 0.970000 | ; factor by which basal water pressure is reduced by thickness effect |
| till_c_0 | 0 | kPa; cohesion of till; note Schoof uses zero but Paterson pp 168--169 gives range 0--40 kPa; but Paterson notes that '... all the pairs c_0 and phi in the table would give a yield stress for Ice Stream B that exceeds the basal shear stress there...' |
| till_pw_fraction | 0.950000 | pure number; pore water pressure is this fraction of overburden |
| viewer_size | 320 | ; default diagnostic viewer size |
| warm_base_flux_enthalpy_fraction | 0.000100 | pure number; in enthalpy model, if base of ice is warmer than pressure-melting, but the enthalpy is within this fraction of L (latent heat of fusion), then some heat flux enters the ice |
| water_latent_heat_fusion | 334000 | J kg-1; latent heat of fusion for water [AschwandenBlatter] |
| water_melting_temperature | 273.150000 | Kelvin; triple point of pure water |
| water_specific_heat_capacity | 4170 | J kg-1 Kelvin-1; at triple point T_0 [AschwandenBlatter] |