Changeset 3342
- Timestamp:
- 2012-04-02T15:41:34+02:00 (12 years ago)
- Location:
- branches/2012/dev_r3337_NOCS10_ICB/DOC/TexFiles
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- 1 added
- 1 edited
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branches/2012/dev_r3337_NOCS10_ICB/DOC/TexFiles/Chapters/Chap_SBC.tex
r3294 r3342 1 1 % ================================================================ 2 % Chapter Ñ Surface Boundary Condition (SBC )3 % ================================================================ 4 \chapter{Surface Boundary Condition (SBC ) }2 % Chapter Ñ Surface Boundary Condition (SBC, ICB) 3 % ================================================================ 4 \chapter{Surface Boundary Condition (SBC, ICB) } 5 5 \label{SBC} 6 6 \minitoc … … 56 56 Next the scheme for interpolation on the fly is described. 57 57 Finally, the different options that further modify the fluxes applied to the ocean are discussed. 58 One of these is modification by icebergs (see \S\ref{ICB_icebergs}), which act as drifting sources of fresh water. 58 59 59 60 … … 1045 1046 the expense of having more idle CICE processors in areas where there is no sea ice. 1046 1047 1048 % ------------------------------------------------------------------------------------------------------------- 1049 % Handling of icebergs 1050 % ------------------------------------------------------------------------------------------------------------- 1051 \subsection{ Handling of icebergs (ICB) } 1052 \label{ICB_icebergs} 1053 %------------------------------------------namberg---------------------------------------------------- 1054 \namdisplay{namberg} 1055 %------------------------------------------------------------------------------------------------------------- 1056 1057 Icebergs are modelled as lagrangian particles in NEMO. 1058 Their physical behaviour is controlled by equations as described in Martin and Adcroft (2010). 1059 (Note that the authors kindly provided a copy of their code to act as a basis for implementation in NEMO.) 1060 Icebergs are initially spawned into one of ten classes which have specific mass and thickness as described by 1061 \np{rn\_initial\_mass} and \np{rn\_initial\_thickness}. 1062 Each class has an associated scaling (\np{rn\_mass\_scaling}), which is an integer representing how many icebergs 1063 of this class are being described as one lagrangian point (this reduces the numerical problem of tracking every single iceberg). 1064 They are enabled by setting \np{ln\_icebergs}~=~true. 1065 1066 Two initialisation schemes are possible. 1067 \begin{description} 1068 \item[\np{nn\_test\_icebergs}~>~0] 1069 In this scheme, the value of \np{nn\_test\_icebergs} represents the class of iceberg to generate (so between 1 and 10), and 1070 \np{nn\_test\_icebergs} provides a lon/lat box in the domain at each grid point of which an iceberg is generated at the 1071 beginning of the run. (Note that this happens each time the timestep equals \np{nn\_nit000}.) 1072 \np{nn\_test\_icebergs} is defined by four numbers in \np{nn\_test\_box} representing the corners of the geographical 1073 box: lonmin,lonmax,latmin,latmax 1074 \item[\np{nn\_test\_icebergs}~=~-1] 1075 In this scheme the model reads a calving file supplied in the \np{sn\_icb} parameter. 1076 This should be a file with a field on the configuration grid (typically ORCA) representing ice accumulation rate at each model point. 1077 These should be ocean points adjacent to land where icebergs are known to calve. 1078 Most points in this input grid are going to have value zero. 1079 When the model runs, ice is accumulated at each grid point which has a non-zero source term. 1080 At each time step, a test is performed to see if there is enough ice mass to calve an iceberg of each class in order (1 to 10). 1081 Note that this is the initial mass multiplied by the number each particle represents (i.e. the scaling). 1082 If there is enough ice, a new iceberg is spawned and the total available ice reduced accordingly. 1083 \end{description} 1084 1085 Icebergs are influenced by wind, waves and currents, bottom melt and erosion. 1086 The latter act to disintegrate the iceberg. 1087 This is either all melted freshwater, or (if \np{rn\_bits\_erosion\_fraction}~>~0) into melt and additionally small ice bits 1088 which are assumed to propagate with their larger parent and thus delay fluxing into the ocean. 1089 Melt water (and other variables on the configuration grid) are written into the main NEMO model output files. 1090 1091 Extensive diagnostics can be produced. 1092 Separate output files are maintained for human-readable iceberg information. 1093 A separate file is produced for each processor (independent of \np{ln\_ctl}). 1094 The amount of information is controlled by two integer parameters: 1095 \begin{description} 1096 \item[\np{nn\_verbose\_level}] takes a value between one and four and represents an increasing number of points in the code 1097 at which variables are written, and an increasing level of obscurity. 1098 \item[\np{nn\_verbose\_level}] is the number of timesteps between writes 1099 \end{description} 1100 1101 Iceberg trajectories can also be written out and this is enabled by setting \np{nn\_sample\_rate}~>~0. 1102 A non-zero value represents how many timesteps between writes of information into the output file. 1103 These output files are in NETCDF format. 1104 When \key{mpp\_mpi} is defined, each output file contains only those icebergs in the corresponding processor, 1105 so care is needed to recreate data for individual icebergs. 1047 1106 1048 1107 % -------------------------------------------------------------------------------------------------------------
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