6.14. jules_snow.nml
¶
This file sets the snow options and parameters. It contains one namelist called JULES_SNOW
.
6.14.1. JULES_SNOW
namelist members¶
HCTN30 refers to Hadley Centre technical note 30, available from the Met Office Library.
- JULES_SNOW::nsmax¶
- Type:
integer
- Permitted:
>= 0
- Default:
0
Maximum possible number of snow layers.
- 0
A composite soil/snow layer is used. This value gives the behaviour found in JULES2.0 and earlier.
- > 0
The state of up to
nsmax
separate snow layers is modelled. Values ofnsmax = 3
or more are recommended.
- JULES_SNOW::l_snowdep_surf¶
- Type:
logical
- Default:
F
- TRUE
Use equivalent canopy snow depth for surface calculations on surface tiles with a snow canopy.
- FALSE
No effect.
- JULES_SNOW::frac_snow_subl_melt¶
- Type:
integer
- Permitted:
0 or 1
- Default:
0
Switch for use of snow-cover fraction in the calculation of sublimation and melting.
Off
On
- JULES_SNOW::graupel_options¶
- Type:
integer
- Permitted:
0, 1 or 2
- Default:
0
Switch for treatment of graupel in the snow scheme
Include graupel as snowfall
Ignore graupel in the surface snowfall
Treat graupel separately
Always “Include graupel as snowfall” (option 0) in standalone JULES because separate snow and graupel driving data are not available. If graupel is included in the UM surface snowfall diagnostic then JULES can either include this graupel as snow in the surface scheme (option 0), ignore this graupel completely, thereby breaking conservation of water and energy in the coupled land-atmosphere model (option 1) or treat graupel separately (currently this only means allowing graupel to fall straight through the canopy)
- JULES_SNOW::dzsnow¶
- Type:
real(nsmax)
- Default:
None
Prescribed thickness of each snow layer (m).
Only used if
nsmax
> 0.The interpretation of
dzsnow
is slightly complicated and an example of the evolution of the snow layers is given below.dzsnow
gives the thickness of each layer when it is not the bottom layer.For the top layer, the minimum thickness is
dzsnow(1)
and the maximum thickness is2 * dzsnow(1)
. For all other layersiz
, the minimum thickness isdzsnow(iz - 1)
, i.e. the given thickness of the previous layer, and the maximum thickness is2 * dzsnow(iz)
, i.e. twice the layerdzsnow
value, except for the last possible layer (nsmax
) which has no upper limit.As a snowpack deepens, the bottom layer (closest to the soil; label this as layer
b
) thickens until it reaches its maximum allowed thickness, at which point it will split into a layer of depthdzsnow(b)
and a new bottom layerb + 1
is added to hold the remaining snow. If a layer becomes thinner than its value indzsnow
it is removed and the snow partitioned between the remaining layers. Whenever a layer splits or is removed, the properties of the layer (e.g. temperature) are allocated to the remaining layers.Note that
dzsnow(nsmax)
, the final thickness, is not used but a value must be input.
- JULES_SNOW::cansnowpft¶
- Type:
logical(npft)
- Default:
F
Flag indicating whether snow can be held under the canopy of each PFT.
Only used if
can_model
= 4.The model of snow under the canopy is currently only suitable for trees.
- TRUE
Snow can be held under the canopy.
- FALSE
Snow cannot be held under the canopy.
Radiation parameters
- JULES_SNOW::r0¶
- Type:
real
- Default:
50.0
Grain size for fresh snow (μm).
Only used if
l_snow_albedo
= TRUE orl_embedded_snow
= TRUE.
- JULES_SNOW::rmax¶
- Type:
real
- Default:
2000.0
Maximum snow grain size (μm).
Only used if
l_snow_albedo
= TRUE orl_embedded_snow
= TRUE.
- JULES_SNOW::snow_ggr¶
- Type:
real(3)
- Default:
0.6, 0.06, 0.23e6
Snow grain area growth rates (μm2 s-1).
Only used if
l_snow_albedo
= TRUE orl_embedded_snow
= TRUE, and requires a snow grain size to calculate the albedo.The three values are for melting snow, cold fresh snow and cold aged snow respectively, the use of which depends on the setting
i_grain_growth_opt
as follows:Growth rates used
Notes
0
snow_ggr
(1:3)Uses all values; melting snow, cold fresh snow and cold aged snow
1
snow_ggr
(1)Uses values for melting snow only.
For cold snow a separate scheme is used following Taillandier et al. (2007), where the parameters are currently hard-wired.
- JULES_SNOW::amax¶
- Type:
real(2)
- Default:
0.98, 0.7
Maximum albedo for fresh snow.
Only used if
l_snow_albedo
orl_elev_land_ice
is TRUE.Values 1 and 2 are for VIS and NIR wavebands respectively.
When:
l_snow_albedo
= TRUEThese parameters are used as limits at all snow-covered grid points.
l_embedded_snow
= TRUEThese parameters are not used.
l_elev_land_ice
= TRUEIrrespective of whether either of the two previous options are selected, these parameters are used to adjust the albedo of dense snow to a value more appropriate for firn. See also
aicemax
.
- JULES_SNOW::aicemax¶
- Type:
real(2)
- Default:
0.78, 0.36
Maximum albedo for bare ice
Only used if
l_elev_land_ice
= TRUE. See alsorho_firn_albedo
.Values 1 and 2 are for VIS and NIR wavebands respectively.
- JULES_SNOW::maskd¶
- Type:
real
- Default:
50.0
Used in the calculation of the weighting factor for snow in the setting of the overall surface albedo, the surface resistance and surface melting. It represents the inverse of the e-folding depth for masking by snow. A higher value indicates that masking by snow is more effective.
N.B. This was originally used to multiply the snow mass (with a standard value of 0.2), but is now used to multiply the snow depth.
- JULES_SNOW::dtland¶
- Type:
real
- Default:
2.0
Degrees Celsius below zero at which snow albedo equals cold deep snow albedo.
This is used only if the diagnostic snow albedo scheme is selected, i.e. if
l_snow_albedo
= FALSE andl_embedded_snow
= FALSE. This is 2.0 in HCTN30 Eq4.Must not be zero.
- JULES_SNOW::kland_numerator¶
- Type:
real
- Default:
0.3
Used in snow-ageing effect on albedo.
This is used only if the diagnostic snow albedo scheme is selected, i.e. if
l_snow_albedo
= FALSE andl_embedded_snow
= FALSE. This is 2.0 in HCTN30 Eq4.kland
is computed by dividing this value bydtland
- see HCTN30 Eq4.
- JULES_SNOW::can_clump¶
- Type:
real(npft)
- Default:
MDI
Clumping parameter for snow on the canopy in calculation of albedo.
Only used if
can_model
= 4,l_embedded_snow
= TRUE andcansnowpft
= TRUE on that surface tile.The model of snow under the canopy is currently only suitable for trees.
The inverse of this parameter specifies the fraction of the canopy over which snow is distributed when calculating the albedo. It should not be less than 1 and higher values indicate that snow on a canopy is more clumped, leaving more of the bare canopy exposed.
- JULES_SNOW::n_lai_exposed¶
- Type:
real(npft)
- Default:
MDI
LAI distribution parameter for calculation of snow albedo.
A power-law distribution of leaf area density is assumed within the canopy for calculating masking of snow by vegetation using the embedded scheme. Higher values indicate that snow is more effective in covering vegetation.
Only used if
l_embedded_snow
= TRUE.
- JULES_SNOW::lai_alb_lim_sn¶
- Type:
real(npft)
- Default:
MDI
Minimum LAI in calculation of albedo in the presence of snow.
A minimum albedo is imposed when calculating the albedo of plant canopies (historically 0.5). This parameter allows it to be set for each PFT in the presence of snow. Crudely, it represents the stem area of vegetation remaining when the true LAI is 0. A separate variable,
lai_alb_lim_io
is used in the absence of snow.
Other snow parameters
- JULES_SNOW::rho_snow_const¶
- Type:
real
- Default:
250.0
Constant density of lying snow (kg m-3).
If
nsmax
= 0, snow is modelled as a single layer of constant density using this value.If
nsmax
> 0, snow density is prognostic, except for snow on the canopy whencansnowpft
is TRUE, and for thin layers of snow whennsmax
> 0.
- JULES_SNOW::rho_snow_fresh¶
- Type:
real
- Default:
100.0
Density of fresh snow (kg m-3).
Only used if
nsmax
> 0.
- JULES_SNOW::rho_firn_albedo¶
- Type:
real
- Default:
550.0
Only used if
l_elev_land_ice
= TRUE.This is the threshold density (as measured over the ~top 10 cm, depending on how the
dzsnow
layers are specified) at which the grain-size calculation of prognostic snow albedo will switch to one dependent on the surface density of the snowpack. Albedo is linearly scaled betweenamax
forrho_snow_const
andaicemax
for density the of ice (917 kg m-3).
- JULES_SNOW::snow_hcon¶
- Type:
real
- Default:
0.265
Thermal conductivity of lying snow (W m-1 K-1).
This value is used for all snow if
nsmax
= 0, but only for thin snow ifnsmax
> 0. See HCTN30 Eq.42. for its application.
- JULES_SNOW::snow_hcap¶
- Type:
real
- Default:
0.63e6
Thermal capacity of lying snow (J K-1 m-3).
- JULES_SNOW::snowliqcap¶
- Type:
real
- Default:
0.05
Liquid water holding capacity of lying snow, as a fraction of snow mass.
Only used if
nsmax
> 0.
- JULES_SNOW::snowinterceptfact¶
- Type:
real
- Default:
0.7
Constant in relationship between mass of intercepted snow and snowfall rate.
Only used if
can_model
= 4.
- JULES_SNOW::snowloadlai¶
- Type:
real
- Default:
4.4
Ratio of maximum canopy snow load to leaf area index (kg m-2).
Only used if
can_model
= 4.
- JULES_SNOW::snowunloadfact¶
- Type:
real
- Default:
0.4
Constant in relationship between canopy snow unloading and canopy snow melt rate.
Only used if
can_model
= 4.
- JULES_SNOW::unload_rate_cnst¶
- Type:
real(npft)
- Default:
MDI
Constant term in the background unloading rate for snow on the canopy. Snow is unloaded from the canopy as a background process or because it is melting.
Only used if
can_model
= 4 andcansnowpft
= TRUE on that surface tile.
- JULES_SNOW::unload_rate_u¶
- Type:
real(npft)
- Default:
MDI
Term proportional to wind speed in the background unloading rate for snow on the canopy.
Only used if
can_model
= 4 andcansnowpft
= TRUE on that surface tile.
- JULES_SNOW::i_snow_cond_parm¶
- Type:
integer
- Permitted:
0 or 1
- Default:
MDI
Scheme used to calculate the conductivity of snow
Only used if
nsmax
> 0.Two parametrizations of snow conductivity are available taken from the papers of Yen (1981) and Calonne et al. (2011).
- JULES_SNOW::l_et_metamorph¶
- Type:
logical
- Default:
F
This parametrization follows the form used by e.g. Dutra et al. (2010).
Only used if
nsmax
> 0.- TRUE
Include the effect of thermal metamorphism on the snow density.
- FALSE
No effect.
- JULES_SNOW::l_snow_infilt¶
- Type:
logical
- Default:
F
Only used if
nsmax
> 0.- TRUE
Pass rainfall and melting from the canopy to the snowpack as infiltration.
- FALSE
No effect.
- JULES_SNOW::l_snow_nocan_hc¶
- Type:
logical
- Default:
F
Only used if
nsmax
> 0.- TRUE
Do not include the canopy heat capacity in the surface energy balance at the top of the snow pack on surface tiles without a canopy snow model.
- FALSE
The canopy heat capacity is included in the surface energy balance at the top of the snow pack.
- JULES_SNOW::a_snow_et¶
- Type:
real
- Default:
MDI
Constant in parametrization of thermal metamorphism.
Only used if
l_et_metamorph
= TRUE.
- JULES_SNOW::b_snow_et¶
- Type:
real
- Default:
MDI
Constant in parametrization of thermal metamorphism.
Only used if
l_et_metamorph
= TRUE.
- JULES_SNOW::c_snow_et¶
- Type:
real
- Default:
MDI
Constant in parametrization of thermal metamorphism.
Only used if
l_et_metamorph
= TRUE.
- JULES_SNOW::rho_snow_et_crit¶
- Type:
real
- Default:
MDI
Critical density in parametrization of thermal metamorphism.
Only used if
l_et_metamorph
= TRUE.
- JULES_SNOW::i_grain_growth_opt¶
- Type:
integer
- Permitted:
0 or 1
- Default:
0
Scheme used to calculate the rate of growth of snow grains.
Invokes the original scheme based on Marshall (1989), with no dependence of the rate of growth of small grains on the temperature.
Invokes the scheme for growth of snow grains proposed by Taillandier et al. (2007) for equitemperature metamorphism. Growth is significantly slower than the default scheme at low temperatures.
- JULES_SNOW::i_relayer_opt¶
- Type:
integer
- Permitted:
0 or 1
- Default:
0
Scheme used to relayer the snowpack.
Only used if
nsmax
> 0.Invokes the original scheme with relayering of the grain size involving the grain size itself.
Relayering is done using the inverse of the grain size. This is more consistent with conserving the specific surface area of snow, though full conservation would require mass weighting to be invoked during regridding.
- JULES_SNOW::i_basal_melting_opt¶
- Type:
integer
- Permitted:
0 or 1
- Default:
0
Option to treat basal melting of the snow pack.
When snow falls on warm ground, it will melt from the base of the snowpack, where the temperature of the snow will rise to the melting point. The 0-layer snow scheme, which is used for thin snow even when the multilayer scheme is selected, did not represent this process and included only melting at the surface.
Default: Basal melting is omitted.
Basal melting takes place instantaneously if the temperature of the first soil layer is above freezing, until the snow is removed or the temperature of soil layer is reduced to freezing.
6.14.2. Example of the evolution of snow layer thickness¶
The table below gives an example of how the number and thickness of snow layers varies with total snow depth for the case of nsmax
= 3 and dzsnow = (0.1, 0.15, 0.2)
. Note that if the values given by the user for dzsnow
are a decreasing series with dzsnow(i) <= 2 * dzsnow(i - 1)
, the algorithm will result in layers i
and i + 1
being added at the same time. Don’t panic - this should not be a problem for the simulation.
Snow depth (m) |
Number of layers |
Layer thickness, uppermost layer first (m) |
Comments |
---|---|---|---|
|
0 |
While the depth of snow is less than |
|
|
1 |
Total snow depth |
The single layer grows until it is twice as thick as |
|
2 |
0.1, remainder |
Above 0.2m, the single layer splits into a top layer of 0.1m and the remaining snow in the bottom layer. |
|
3 |
0.1, 0.15, remainder |
At 0.4m depth, layer 2 (which has grown to 0.3m thick, i.e. |
6.14.3. JULES_SNOW
references¶
Calonne, N., Flin, F., Morin, S., Lesaffre, B., du Roscoat, S. Rolland, and Geindreau, C. (2011). Numerical and experimental investigations of the effective thermal conductivity of snow, Geophys. Res. Lett., 38, L23501, https://doi.org/10.1029/2011GL049234.
Dutra, E., Balsamo, G., Viterbo, P., Miranda, P. M., Beljaars, A., Schar, C., and Elder, K. (2010). An improved snow scheme for the ECMWF land surface model: Description and offline validation, J. Hydrometeorol., 11, 899–916, https://doi.org/10.1175/2010JHM1249.1.
Marshall, S.E. (1989). A physical parameterization of snow albedo for use in climate models. NCAR Cooperative Thesis 123. Boulder, CO : National Center for Atmospheric Research. https://atmos.washington.edu/~sgw/PAPERS/1989_Marshall.pdf
Taillandier, A.-S., F. Domine, W. R. Simpson, M. Sturm, and T. A. Douglas (2007). Rate of decrease of the specific surface area of dry snow: Isothermal and temperature gradient conditions, J. Geophys. Res., 112, F03003, https://doi.org/10.1029/2006JF000514.
Yen, Y.-C. (1981). Review of thermal properties of snow, ice and sea ice. Cold Regions Research and Engineering Laboratory (CRREL) Report 81-10. https://hdl.handle.net/11681/9469