definitions.py
55b3f0fbb1cf2Dhandling

definitions.py
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			from __future__ import division, print_function
			###########################################################################
			# #
			# Copyright 2017 Andrea Cimatoribus #
			# EPFL ENAC IIE ECOL #
			# GR A1 435 (Batiment GR) #
			# Station 2 #
			# CH-1015 Lausanne #
			# Andrea.Cimatoribus@epfl.ch #
			# #
			# This file is part of ctracker #
			# #
			# ctracker is free software: you can redistribute it and/or modify it #
			# under the terms of the GNU General Public License as published by #
			# the Free Software Foundation, either version 3 of the License, or #
			# (at your option) any later version. #
			# #
			# ctracker is distributed in the hope that it will be useful, #
			# but WITHOUT ANY WARRANTY; without even the implied warranty #
			# of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. #
			# See the GNU General Public License for more details. #
			# #
			# You should have received a copy of the GNU General Public License #
			# along with ctracker. If not, see <http://www.gnu.org/licenses/>. #
			# #
			###########################################################################

			#
			# MITgcm results description
			#

			# Directory containing the hydrodynamics fields
			gcm_directory = "/home/cimatori/Work/mitgcm/lac_leman/run_2016"

			# u-velocity filename root
			u_root = "UVEL"
			# v-velocity filename root
			v_root = "VVEL"
			# w-velocity filename root
			w_root = "WVEL"

			# output data type (">f8" for double precision, ">f4" for single)
			out_prec = ">f4"

			# grid geometry used in the MITgcm simulation
			gcm_geometry = "curvilinear"

			# reference date of MITgcm simulation
			gcm_start = "2013-11-12 12:00"

			# MITgcm time step in seconds
			gcm_dt = 20.0

			# MITgcm output time step in seconds
			out_dt = 1800.0


			#
			# Simulation configuration
			#

			# file name for output (netcdf)
			outfile = "/tmp/test.nc"

			# start date of particle tracking simulation
			start = "2015-12-12 12:30"

			# end date of particle tracking simulation
			end = "2015-12-13 12:30"

			# list of seed points coordinates
			x_seed = [553319.0]
			y_seed = [137896.0]
			z_seed = [2.5]

			# if inds_seed is True, x_seed, y_seed and z_seed are
			# given in terms of (fractional) indices, otherwise they
			# are interpreted as being in the same units as the MITgcm grid
			inds_seed = False

			# Note that seeding only takes place at the GCM output time
			# If you pass the wrong time, no seeding will take place.
			# seeding start time
			seed_start = "2015-12-12 12:30"

			# seeding end time
			seed_end = "2015-12-12 12:31"

			# seeding interval in seconds
			seed_interval = 1800

R3351/ctracker/definitions.py55b3f0fbb1cf2Dhandling

definitions.pyView Options

R3351/ctracker/definitions.py
55b3f0fbb1cf2Dhandling

definitions.py
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