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To reference or cite the objects present in the Software Heritage archive, permalinks based on SoftWare Hash IDentifiers (SWHIDs) must be used.
Select below a type of object currently browsed in order to display its associated SWHID and permalink.

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swh:1:cnt:a7a78f9b1e9a56537cf376ae428e9a5aef2a1222

This interface enables to generate software citations, provided that the root directory of browsed objects contains a citation.cff or codemeta.json file.
Select below a type of object currently browsed in order to generate citations for them.

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Generate software citation in BibTex format (requires biblatex-software package)
Generating citation ...
#!/usr/bin/env python
# coding: utf-8

# ## Reinhold and Pierrehumbert 1982 model version

# This model version is a simple 2-layer channel QG atmosphere truncated at wavenumber 2 on a beta-plane with
# a simple orography (a montain and a valley).
# 
# More detail can be found in the articles:
# 
# * Reinhold, B. B., & Pierrehumbert, R. T. (1982). Dynamics of weather regimes: Quasi-stationary waves and blocking.
#   Monthly Weather Review, 110(9), 1105-1145.
# * Cehelsky, P., & Tung, K. K. (1987). Theories of multiple equilibria and weather regimes—A critical reexamination.
#   Part II: Baroclinic two-layer models. Journal of the atmospheric sciences, 44(21), 3282-3303.


# ## Modules import
import numpy as np
import sys
import time
from multiprocessing import freeze_support, get_start_method

# Importing the model's modules
from qgs.params.params import QgParams
from qgs.integrators.integrator import RungeKuttaIntegrator
from qgs.functions.tendencies import create_tendencies

# Initializing the random number generator (for reproducibility). -- Disable if needed.
np.random.seed(21217)

if __name__ == "__main__":

    if get_start_method() == "spawn":
        freeze_support()

    print_parameters = True


    def print_progress(p):
        sys.stdout.write('Progress {:.2%} \r'.format(p))
        sys.stdout.flush()


    class Bcolors:
        """to color the instructions in the console"""
        HEADER = '\033[95m'
        OKBLUE = '\033[94m'
        OKGREEN = '\033[92m'
        WARNING = '\033[93m'
        FAIL = '\033[91m'
        ENDC = '\033[0m'
        BOLD = '\033[1m'
        UNDERLINE = '\033[4m'


    print("\n" + Bcolors.HEADER + Bcolors.BOLD + "Model qgs v1.0.0 (Atmosphere + orography configuration)" + Bcolors.ENDC)
    print(Bcolors.HEADER + "=======================================================" + Bcolors.ENDC + "\n")
    print(Bcolors.OKBLUE + "Initialization ..." + Bcolors.ENDC)
    # ## Systems definition

    # General parameters

    # Time parameters
    dt = 0.1
    # Saving the model state n steps
    write_steps = 5
    # transient time to attractor
    transient_time = 1.e5
    # integration time on the attractor
    integration_time = 1.e4
    # file where to write the output
    filename = "evol_fields.dat"
    T = time.process_time()

    # Setting some model parameters
    # Model parameters instantiation with some non-default specs
    model_parameters = QgParams({'phi0_npi': np.deg2rad(50.)/np.pi, 'hd': 0.1})
    # Mode truncation at the wavenumber 2 in both x and y spatial coordinate
    model_parameters.set_atmospheric_channel_fourier_modes(2, 2)

    # Changing (increasing) the orography depth and the meridional temperature gradient
    model_parameters.ground_params.set_orography(0.2, 1)
    model_parameters.atemperature_params.set_thetas(0.2, 0)

    if print_parameters:
        print("")
        # Printing the model's parameters
        model_parameters.print_params()

    # Creating the tendencies functions
    f, Df = create_tendencies(model_parameters)

    # ## Time integration
    # Defining an integrator
    integrator = RungeKuttaIntegrator()
    integrator.set_func(f)

    # Start on a random initial condition
    ic = np.random.rand(model_parameters.ndim)*0.1
    # Integrate over a transient time to obtain an initial condition on the attractors
    print(Bcolors.OKBLUE + "Starting a transient time integration..." + Bcolors.ENDC)
    ws = 1000
    y = ic
    total_time = 0.
    t_up = ws * dt / integration_time * 100
    while total_time < transient_time:
        integrator.integrate(0., ws * dt, dt, ic=y, write_steps=0)
        t, y = integrator.get_trajectories()
        total_time += t
        if total_time/transient_time * 100 % 0.1 < t_up:
            print_progress(total_time/transient_time)

    # Now integrate to obtain a trajectory on the attractor
    total_time = 0.
    traj = np.insert(y, 0, total_time)
    traj = traj[np.newaxis, ...]
    t_up = write_steps * dt / integration_time * 100

    print(Bcolors.OKBLUE + "Starting the time evolution ..." + Bcolors.ENDC)
    while total_time < integration_time:
        integrator.integrate(0., write_steps * dt, dt, ic=y, write_steps=0)
        t, y = integrator.get_trajectories()
        total_time += t
        ty = np.insert(y, 0, total_time)
        traj = np.concatenate((traj, ty[np.newaxis, ...]))
        if total_time/integration_time*100 % 0.1 < t_up:
            print_progress(total_time/integration_time)

    print(Bcolors.OKGREEN + "Evolution finished, writing to file " + filename + Bcolors.ENDC)

    np.savetxt(filename, traj)

    print(Bcolors.OKGREEN + "Time clock :" + Bcolors.ENDC)
    print(str(time.process_time()-T)+' seconds')

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