Beispiel #1
0
def plot_volume(in_dict, time_array, route, o_dir, case_name):
    #----parameters----#
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    year = 365 * 24 * 3600
    time_scaling = pow(Ro, 2.0) / Kappa / (1e6 * year)
    melt_scaling = pow(Ro, 3.0) / 1e9
    v_file = '%s/%s.volume.dat' % (route, case_name)
    if os.path.isfile(v_file) is False:
        print('no file %s' % (v_file))
        return
    #----read data----#
    v_data, v_steps = readf.read_q_file(v_file, time_array, 6)
    v_time = v_data[:, 0] * time_scaling
    v_T = v_data[:, 1]
    v_melt = v_data[:, 5] * melt_scaling
    #print(v_time) #debug
    #print(v_T) #debug
    #----plot figures----#
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    o_dir = Mpf.assign_output_dir("%s/vol" % (case_dir))
    fig, ax = plt.subplots()
    ax = plt.subplot(2, 1, 1)
    plt.plot(v_time, v_T, 'r-')
    ax.set(ylabel='Temperature[1.0]')
    ax = plt.subplot(2, 1, 2)
    plt.plot(v_time, v_melt, 'c-')
    ax.set(xlabel='Time [ma]', ylabel='Total melt volume [km^3]')
    fig.savefig("%s/volume_value.eps" % (o_dir))
    plt.close(fig)
Beispiel #2
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def hoz_combine(in_dict, route, cname, ta, steps, hdict):
    fname = '%s_hoz_combine' % (cname)
    dir0 = './gmt'
    temp = hdict['temp']
    rho = hdict['rho']
    col = hdict['col']
    nprocz = readf.get_variable(in_dict, 'nprocz', 'int')
    noz = readf.get_variable(in_dict, 'nodez', 'int')
    lnoz = int((noz - 1) / nprocz) + 1
    foname = '%s/%s' % (dir0, fname)
    if os.path.isfile(foname):
        os.remove(foname)
    for i in range(len(steps)):
        step = steps[i]
        t = ta[step]
        for pz in range(nprocz):
            filename = '%s/%s.horiz_avg.%d.%d' % (route, cname, pz, step)
            data = readf.read_data(filename)
            with open(foname, 'a') as fo:
                for lnz in range(lnoz):
                    if pz >= 1 and lnz == 0:
                        continue
                    nn = lnz * col
                    fo.write('%.4e %.4e %.4e %.4e\n' %
                             (t, data[nn], data[nn + temp], data[nn + rho]))
    return fname
Beispiel #3
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 def __init__(self, _paraDict, _colsDict, _stepsTuple):
     self.cD = _colsDict
     self.sT = _stepsTuple
     self.dataFile = _paraDict['datafile']
     Ro = readf.get_variable(_paraDict, 'radius', 'float')
     Kappa = readf.get_variable(_paraDict, 'thermdiff', 'float')
     self.tScale = Ro**2.0 / Kappa / (1e6 * year)
Beispiel #4
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def LowerMantle(_paraDict):
    tiny = 1e-6
    Range = []
    ro = readf.get_variable(_paraDict, 'radius_outer', 'float')
    ri = readf.get_variable(_paraDict, 'radius_inner', 'float')
    Range.append(ri - tiny)
    Range.append((ri + ro) / 2.0 + tiny)
    return Range
Beispiel #5
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def IbcLayer(_paraDict):
    Range = []
    IbcInterfaceIndex = 1
    blur = 0.8
    InterF = readf.get_variable(_paraDict, 'z_interface', 'float_list')
    zLith = readf.get_variable(_paraDict, 'z_lith', 'float')
    ro = readf.get_variable(_paraDict, 'radius_outer', 'float')
    upper = ro - zLith
    lower = InterF[IbcInterfaceIndex]
    thick = upper - lower
    Range.append(lower - blur * thick)
    Range.append(upper + blur * thick)
    return Range
Beispiel #6
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def plot_volume_1(in_dict, time_array, route, o_dir, case_name, settings):
    #----parameters----#
    column_dict = settings['column']
    color_dict = settings['color']
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    year = 365 * 24 * 3600
    time_scaling = pow(Ro, 2.0) / Kappa / (1e6 * year)
    melt_scaling = pow(Ro, 3.0) / 1e9
    v_file = '%s/%s.volume.dat' % (route, case_name)
    if os.path.isfile(v_file) is False:
        print('no file %s' % (v_file))
        return
    data = readf.read_data_1(v_file)
    temp = column_dict['step']
    step_array = data[:, temp]
    xdata = np.zeros(step_array.shape)
    for n in range(step_array.size):
        step = int(step_array[n])
        xdata[n] = time_array[step] * time_scaling
    #----plot figures----#
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    o_dir = Mpf.assign_output_dir("%s/vol" % (case_dir))
    fig, ax = plt.subplots()
    #----temperature----#
    ax = plt.subplot(2, 1, 1)
    temp = column_dict['temp']
    ydata = data[:, temp]
    color_type = color_dict['temp']
    plt.plot(xdata, ydata, color=color_type, linestyle='-', label='average T')
    ax.legend()
    ax.set(ylabel='Temperature[1.0]')
    #----melting----#
    ax = plt.subplot(2, 1, 2)
    temp = column_dict['melting'][0]
    color_type = color_dict['melting'][0]
    n_c = len(column_dict['melting']) - 1
    ydata = data[:, temp] * melt_scaling
    plt.plot(xdata, ydata, color=color_type, linestyle='-', label='total')
    for n in range(n_c):
        name = 'chemical %d' % (n)
        temp = column_dict['melting'][n + 1]
        ydata = data[:, temp] * melt_scaling
        color_type = color_dict['melting'][n + 1]
        plt.plot(xdata, ydata, color=color_type, linestyle='--', label=name)
    ax.legend()
    ax.set(xlabel='Time [ma]', ylabel='Total melt volume [km^3]')
    fig.savefig("%s/volume_value.eps" % (o_dir))
    plt.close(fig)
Beispiel #7
0
def magnetism_intensiy(in_dict, q_data, Tc):
    pi = np.pi
    G = 6.67e-11
    alphac = 6e-5
    rhoc = 7400
    kc = 40
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    rc = readf.get_variable(in_dict, 'radius_inner', 'float')
    Rc = Ro * rc
    cpc = 800
    f = 1.0 / 7
    fohm = 1.0
    c = 0.63
    mu0 = 4 * pi * 1e-7
    qad = 4 * pi * G * alphac * rhoc * Tc * kc * Rc / (3 * cpc)
    qdiff = (q_data - qad) * (q_data - qad > 0.0)
    B = f * (Rc / Ro)**(3.0) * (2 * mu0 * fohm * c * rhoc**
                                (1.0 / 3))**(0.5) * (qdiff * qad * Rc /
                                                     (kc * Tc))**(1.0 / 3)
    return B, qad
Beispiel #8
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def heat_flux(in_dict, time_array, step_tuple, route, o_dir, case_name,
              **kwargs):
    def _config(name, default):
        try:
            return kwargs[name]
        except KeyError:
            return default

    year = 365 * 24 * 3600
    write_q = readf.get_variable(in_dict, 'write_q_files', 'int')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    Cp = readf.get_variable(in_dict, 'cp', 'float')
    Rho = readf.get_variable(in_dict, 'density', 'float')
    Tref = readf.get_variable(in_dict, 'reftemperature', 'float')
    Tsurf = readf.get_variable(in_dict, 'surftemperature', 'float')
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    o_dir = Mpf.assign_output_dir("%s/heat_flux" % (case_dir))
    Therm_k = Kappa * Cp * Rho
    time_scaling = pow(Ro, 2.0) / Kappa / (1e6 * year)
    hq_scaling = Therm_k * Tref / Ro * 1e3
    #----read data----#
    q_file = "%s/%s.qb.dat" % (route, case_name)
    cols = _config('cols', 5)
    q_data, q_steps = readf.read_q_file(q_file, time_array, cols)
    #for i in q_data[:,0]:
    #    print(i)#debug
    #print(q_steps) #debug
    colt = _config('colt', 0)
    colq = _config('colq', 1)
    colT = _config('colT', 3)
    print(q_data.size)
    q_time = q_data[:, 0] * time_scaling
    #print(q_data[:,0]) #debug
    q_hq = q_data[:, 1] * hq_scaling
    if colT is not None:
        Tc = q_data[:, 3] * Tref + Tsurf
    else:
        Tc = Tref * np.ones(q_time.size) + Tsurf
    B, qad = magnetism_intensiy(in_dict, q_hq / 1e3, Tc)
    qad = qad * 1e3
    B = B * 1e6
    #----plot figures----#
    fig, ax = plt.subplots()
    ax = plt.subplot(2, 1, 1)
    #fig, ax = plt.subplots()
    plt.plot(q_time, q_hq, 'r-')
    ax.set(ylabel='Heat Flux[mw/m3]')
    ax = plt.subplot(2, 1, 2)
    #fig, ax = plt.subplots(212)
    plt.plot(q_time, B, 'b-')
    ax.set(xlabel='Time [ma]', ylabel='Magnetism [/muT]')
    #plt.show()
    fig.savefig("%s/cmb_heatflux.eps" % (o_dir))
    plt.close(fig)
Beispiel #9
0
 def __init__(self, _paraDict, _colsDict, _stepsTuple, _tArray):
     self.cD = _colsDict
     self.sT = _stepsTuple
     self.tA = _tArray
     self.dataFile = _paraDict['datafile']
     self.nProcZ = readf.get_variable(_paraDict, 'nprocz', 'int')
     Alpha = readf.get_variable(_paraDict, 'thermexp', 'float')
     Tref = readf.get_variable(_paraDict, 'reftemperature', 'float')
     self.Rho = readf.get_variable(_paraDict, 'density', 'float')
     self.RhoScale = Alpha * Tref * self.Rho
     self.bA = readf.get_variable(_paraDict, 'buoyancy_ratio', 'float_list')
     Ro = readf.get_variable(_paraDict, 'radius', 'float')
     Kappa = readf.get_variable(_paraDict, 'thermdiff', 'float')
     self.tScale = Ro**2.0 / Kappa / (1e6 * year)
     self.vScale = Kappa / Ro * year * 1e2
Beispiel #10
0
def plot_mf_melting(in_dict, time_array, route, o_dir, case_name, settings):
    #----parameters----#
    column_dict = settings['column']
    color_dict = settings['color']
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    year = 365 * 24 * 3600
    time_scaling = pow(Ro, 2.0) / Kappa / year
    filename = '%s/%s.mf.dat' % (route, case_name)
    if os.path.isfile(filename) is False:
        print('no file %s' % (filename))
        return
    data = np.genfromtxt(filename)
    temp = column_dict['step']
    step_array = data[:, temp]
    temp = column_dict['eular']
    eu_rate = data[:, temp]
    temp = column_dict['tracer']
    csize = len(temp) - 1
    tr_rate = data[:, temp[0]]
    tr_rate_comp = np.zeros((tr_rate.size, csize))
    for i in range(csize):
        tr_rate_comp[:, i] = data[:, temp[i + 1]]
    eu = np.zeros(step_array.size)
    tr = np.zeros(step_array.size)
    tr_comp = np.zeros((step_array.size, csize))
    time = np.zeros(step_array.size)
    dtime = np.zeros(step_array.size)
    for n in range(step_array.size):
        step = int(step_array[n])
        time[n] = time_array[step] * time_scaling
        if n > 0:
            dtime = time[n] - time[n - 1]
            eu[n] = eu[n - 1] + eu_rate[n - 1] * dtime
            tr[n] = tr[n - 1] + tr_rate[n - 1] * dtime
            tr_comp[n, :] = tr_comp[n - 1, :] + tr_rate_comp[n - 1, :] * dtime
    #----plot figures----#
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    o_dir = Mpf.assign_output_dir("%s/melting" % (case_dir))
    fig, ax = plt.subplots()
    #----temperature----#
    ax = plt.subplot(2, 1, 1)
    color_type = color_dict['tracer']
    plt.plot(time / 1e6,
             tr_rate,
             color=color_type,
             linestyle='--',
             label='Tracer Method')
    color_type = color_dict['eular']
    plt.plot(time / 1e6,
             eu_rate,
             color=color_type,
             linestyle='--',
             label='Eular Method')
    color_type = color_dict['melting']
    for i in range(csize):
        plt.plot(time / 1e6,
                 tr_rate_comp[:, i],
                 color=color_type[i + 1],
                 linestyle='-',
                 label='comp%d' % (i))
    ax.set(ylabel='Melting Producting Rate [km^3/yr]')

    ax = plt.subplot(2, 1, 2)
    color_type = color_dict['tracer']
    plt.plot(time / 1e6,
             tr,
             color=color_type,
             linestyle='--',
             label='Tracer Method')
    color_type = color_dict['eular']
    plt.plot(time / 1e6,
             eu,
             color=color_type,
             linestyle='--',
             label='Eular Method')
    color_type = color_dict['melting']
    for i in range(csize):
        plt.plot(time / 1e6,
                 tr_comp[:, i],
                 color=color_type[i + 1],
                 linestyle='-',
                 label='comp%d' % (i))
    ax.legend()
    ax.set(ylabel='Melting Volume[km^3/yr]')
    ax.set(xlabel='time [ma]')
    fig.tight_layout()
    fig.savefig("%s/mml_melting.eps" % (o_dir))
Beispiel #11
0
def remove_extra_file1(route, case_name, in_dict, time_array, step_tuple,
                       step_start, p_file, plogfile):
    caps = 12
    steps_inter = 30
    nprocz = readf.get_variable(in_dict, 'nprocz', 'int')
    nprocx = readf.get_variable(in_dict, 'nprocx', 'int')
    nprocy = readf.get_variable(in_dict, 'nprocy', 'int')
    nproc = caps * nprocx * nprocy * nprocz

    p_dict = readf.read_input(p_file)
    e_steps = readf.get_variable(p_dict, 'episode_steps', 'int_list')
    steps_in = readf.get_variable(p_dict, 'steps_remain', 'int_list')
    length = len(step_tuple)
    time_at_steps = [time_array[step] for step in step_tuple]
    step_end = step_tuple[len(step_tuple) - 1]
    stime = time_array[step_start]
    ftime = time_array[step_end]
    plog = open(plogfile, 'a')
    #----get time of steps that are worth keeping----#
    time_query = []
    for time in np.linspace(stime, ftime, steps_inter):
        time_query.append(time)
    #----get steps that are worth keeping----#
    for time in time_query:
        n = np.argmin(abs(time_at_steps - time))
        step = step_tuple[n]
        if step not in steps_in:
            steps_in.append(step)
    is_see = input('deleting steps: see steps to keep?(y/n)')
    if is_see:
        print(steps_in)
    input()
    #----delete extra files----#
    for n in range(len(step_tuple)):
        step = step_tuple[n]
        if step < step_start:
            continue

#        bash_command = []
#        bash_command.append('rm %s/%s.proc0.%d.vts'%(route,case_name,step))
#        bash_command.append('rm %s/%s.%d.vtm'%(route,case_name,step))
        if step not in steps_in:
            for proc in range(nproc):
                filename = '%s/%s.proc%d.%d.vts' % (route, case_name, proc,
                                                    step)
                if os.path.isfile(filename):
                    os.remove(filename)
                if proc % nprocz is nprocz - 1:
                    filename = '%s/%s.surf.%d.%d' % (route, case_name, proc,
                                                     step)
                    if os.path.isfile(filename):
                        os.remove(filename)
                    filename = '%s/%s.surf_ori.%d.%d' % (route, case_name,
                                                         proc, step)
                    if os.path.isfile(filename):
                        os.remove(filename)
            filename = '%s/%s.surf_sph.%d' % (route, case_name, step)
            if os.path.isfile(filename):
                os.remove(filename)
            filename = '%s/%s.%d.vtm' % (route, case_name, step)
            if os.path.isfile(filename):
                os.remove(filename)
#            readf.run_bash(bash_command)
            plog.write('remove file at step %d\n' % (step))
    plog.close()
    #----write remain steps to p_file----#
    readf.overwrite_to_file(p_file,
                            'steps_remain',
                            steps_in,
                            vtype='int',
                            vvtype='array')
    input()
Beispiel #12
0
def surf_plot(in_dict, route, o_dir, case_name, step, **kwargs):
    def _config(name, default):
        try:
            return kwargs[name]
        except KeyError:
            return default

    gmt_dir = _config('gmt_dir', './gmt')
    rot = _config('rot', None)
    angle = _config('angle', [0.0, 0.0])
    vtype = _config('vtype', 'total')
    cpt = _config('cpt', None)
    check_bound = _config('check_bound', False)
    cc_file = './cc'
    gravacc = readf.get_variable(in_dict, 'gravacc', 'float')
    Rho = readf.get_variable(in_dict, 'density', 'float')
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    Eta = readf.get_variable(in_dict, 'refvisc', 'float')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    if vtype is 'total':
        deg = -1
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    surf_dir = Mpf.assign_output_dir("%s/surf" % (case_dir))
    file0 = '%s/%s.surf0.%d' % (cc_file, case_name, step)
    if rot is None:
        ofile = '%s/topo_%d_%d.ps' % (surf_dir, step, deg)
        file1 = '%s/%s_%d_surf_combine' % (cc_file, case_name, step)
    else:
        ofile = '%s/topo_%d_%drt%d_%d_%d_%d.ps' % (surf_dir, step, deg, rot[0],
                                                   rot[1], angle[0], angle[1])
        file1 = '%s/%s_%d_surf_combine_rt%d_%d_%d_%d' % (
            cc_file, case_name, step, rot[0], rot[1], angle[0], angle[1])
    scl_ang = 180.0 / np.pi
    if deg is -1:
        col = 2
    else:
        col = deg + 2
    scl_topo = Eta * Kappa / Ro**2.0 / (Rho * gravacc)

    topo_minor = 200
    sminor = 500
    smini = 100

    #----combine surf output----#
    if not os.path.isfile(file1):
        readf.write_surf_runfile(in_dict,
                                 route,
                                 case_name,
                                 step,
                                 vtype='total')
        bashcommand = []
        bashcommand.append('%s/images.x %s/runfile' % (cc_file, cc_file))
        if rot is not None:
            bashcommand.append(
                './lib/eula_polar %s %s %s %s %s %s' %
                (file0, file1, rot[0], rot[1], angle[0], angle[1]))
        readf.run_bash(bashcommand)
        if rot is None:
            os.rename(file0, file1)
    #----read head value---#
    with open(file1) as fin:
        sdata = fin.readline().split()
    data = []
    for s in sdata:
        data.append(float(s) * scl_topo)
    try:
        bound = kwargs['bound']  #enlist bound in kwargs to creat a liste
        topomm = [bound[0], bound[1]]  #that stands for boundary value for
        off_topo = bound[2]  #dynamic topography
    except KeyError:  #else take from input
        idat = input('(min,max,offset),reference:(%.4e %.4e %.4e)\n' %
                     (data[0], data[1], data[2]))
        idat = idat.split(',')
        topomm = []
        topomm.append(float(idat[0]))
        topomm.append(float(idat[1]))
        off_topo = float(idat[2])
    if data[0] < topomm[0] or data[1] > topomm[1]:
        print(
            "at step %s, default value for bound is (%.4e %.4e), given is %.4e %.4e"
            % (step, data[0], data[1], topomm[0], topomm[1]))
    if check_bound:
        return data
    try:
        minor = kwargs['minor']  #enlist minor in kwargs to creat a list that
        topo_minor = minor[0]  #stand for interval in color bar, interval of
        sminor = minor[1]  #scale
        smini = minor[2]
    except KeyError:
        isdo = input('change (topo_minor,sminor,smini) value,default is\
            (%.4e %.4e,%.4e),y/n\n' % (topo_minor, sminor, smini))
        if isdo is 'y':
            nval = input('new value:')
            nval = nval.split(',')
            topo_minor = float(nval[0])
            sminor = float(nval[1])
            smini = float(nval[2])

    #----plot figure using gmt----#
    bashcommand = []
    bashcommand.append(
        'gmt nearneighbor -i1[s%.2f],0[s%.2f][o90],%d[s%.2f][o%.2f] -R0/360/-90/90 -I1/1 -S10 -N1 -G%s/topo.grd -V -h1 %s'
        % (scl_ang, -scl_ang, col, scl_topo, off_topo, gmt_dir, file1))
    if cpt is None:
        cpt = '%s/color.cpt' % (gmt_dir)
        bashcommand.append(
            'gmt makecpt -Cno_green -T%.2f/%.2f/%.2f > %s/color.cpt' %
            (topomm[0], topomm[1], topo_minor, gmt_dir))
    else:
        cpt = '%s/%s' % (gmt_dir, cpt)
    bashcommand.append(
        'gmt grdimage %s/topo.grd -R0/360/-90/90 -C%s -JW90/6i -X0.35i -Y6.0i -B120g30/60g30 -K -P > %s'
        % (gmt_dir, cpt, ofile))
    bashcommand.append(
        'gmt psscale -D3.5i/-0.5i/15.0c/0.5ch -C%s -P -O -U -V -B:Topography/m:%.2ff%.2fWSne >> %s'
        % (cpt, sminor, smini, ofile))
    bashcommand.append('gmt psconvert -A -Tj %s' % ofile)
    readf.run_bash(bashcommand)
Beispiel #13
0
def chemical(in_dict, time_array, step_tuple, column_dict, route, o_dir,
             case_name, pp_file):
    get_end = 1
    split = 6
    init_lower_percent = 0.01
    pi = np.pi
    tiny = 1e-8
    year = 365 * 24 * 3600
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    o_dir = Mpf.assign_output_dir("%s/chemical" % (case_dir))
    if os.path.isfile(pp_file):
        pp_dict = readf.read_input(pp_file)
        try:
            pp_dict['end_time']
        except KeyError:
            get_end = 1
        else:
            get_end = 0
    else:
        get_end = 1
    #----read parameters----#
    cols = column_dict['cols']
    nprocz = readf.get_variable(in_dict, 'nprocz', 'int')
    noz = readf.get_variable(in_dict, 'nodez', 'int')
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    interface = readf.get_variable(in_dict, 'z_interface', 'float_list')
    r_inter = interface[-1]
    r_o = readf.get_variable(in_dict, 'radius_outer', 'float')
    r_in = readf.get_variable(in_dict, 'radius_inner', 'float')
    r_lith = r_o - readf.get_variable(in_dict, 'z_lith', 'float')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    r_half = (r_o + r_in) / 2.0
    lnoz = int((noz - 1) / nprocz) + 1
    time_scaling = pow(Ro, 2.0) / Kappa / (1e6 * year)
    total_ibc = 4 * pi / 3 * (pow(r_lith, 3.0) - pow(r_lith - 20e3 / Ro, 3.0))
    #----prepare chemical data----#
    chemical = np.zeros((len(step_tuple), 3))
    time1 = np.zeros(len(step_tuple))
    n = 0
    for step in step_tuple:
        time1[n] = time_array[step]
        print(step, end='\r')
        data_in = readf.read_horig_output(route, case_name, step, nprocz, lnoz,
                                          cols)
        rr = data_in[:, column_dict['radius']]
        C = data_in[:, column_dict['ic']]
        for i in range(noz - 1):
            volume = 4.0 / 3.0 * pi * (pow(rr[i + 1], 3.0) - pow(rr[i], 3.0))
            if rr[i] > r_inter - tiny and rr[i] < r_lith + tiny:
                chemical[n,
                         0] = chemical[n, 0] + (C[i] + C[i + 1]) / 2.0 * volume
            if rr[i] > r_half - tiny:
                chemical[n,
                         1] = chemical[n, 1] + (C[i] + C[i + 1]) / 2.0 * volume
            if rr[i] < r_half + tiny:
                chemical[n,
                         2] = chemical[n, 2] + (C[i] + C[i + 1]) / 2.0 * volume
        n = n + 1
    total_chemical = chemical[0, 1] + chemical[0, 2]
    chemical_low = chemical[:, 2]  #chemical_low is lower chemical percent
    #print(chemical[0,1]+chemical[0,2])
    #print(chemical[:,0]) #debug
    #print(chemical[:,1])
    #print(chemical[:,2])
    #----plot figures----#
    #----figure 1 : retained chemical----#
    fig, ax = plt.subplots()
    line1, = ax.plot(time1 * time_scaling, chemical[:, 0] / chemical[0, 0],
                     'r-')
    ax.set(xlabel='Time [ma]',
           ylabel='Chemical Percent[1]',
           title='Retained Chemicals in Initial Layer')
    fig.savefig("%s/retained_ibc.eps" % (o_dir))
    #plt.show()
    plt.close(fig)
    #----figure 2 : overturned chemical----#
    time2 = time1 * time_scaling
    fig, ax = plt.subplots()
    line1, = ax.plot(time2, chemical_low / total_chemical, 'b-')
    ax.set(xlabel='Time [ma]',
           ylabel='Chemical Percent[1]',
           title='Overturned Chemical')
    fig.savefig("%s/overturned_chemical.eps" % (o_dir))
    #plt.show()
    plt.close(fig)
    #----figure 3 : overturned ibc volume----#
    fig, ax = plt.subplots()
    line1, = ax.plot(time2, chemical_low / total_chemical * total_ibc, 'c-')
    ax.set(xlabel='Time [ma]', ylabel='IBC Volume[1]', title='Overturned IBC')
    fig.savefig("%s/overturned_IBC.eps" % (o_dir))
    if get_end is 1:
        temp = input(
            "input scheme to continue getting end for overturn: 'a(auto)/m(manual):"
        )
        if temp is 'a':
            cid = fig.canvas.mpl_connect('button_press_event', on_press)
            plt.show()
            end_time = get_end_time(Gmc[0], Gmc[1], Gmc[2])
            diff_t = abs(time2 - end_time)
            end_n = np.argmin(diff_t)
            end_c = chemical_low[end_n]
            episode_c = np.linspace(0.0, 1.0, split) * end_c
            episode_c[0] = init_lower_percent * end_c
            episode_steps = []
            for cc in episode_c:
                diff_c = abs(chemical_low - cc)
                tempn = np.argmin(diff_c)
                episode_steps.append(step_tuple[tempn])
            end_c_percent = end_c / total_chemical
            episode_completness = episode_c / end_c
            fig.canvas.mpl_disconnect(cid)
        elif temp is 'm':
            plt.show()
            temp = input('endstep for episode:')
            end_step = int(temp)
            end_time = time_array[end_step] * time_scaling
            diff_t = abs(time2 - end_time)
            end_n = np.argmin(diff_t)
            episode_t = np.linspace(0.0, 1.0, split) * end_time
            end_c = chemical_low[end_n]
            end_c_percent = end_c / total_chemical
            episode_completness = episode_t / end_time
            episode_steps = []
            for tt in episode_t:
                diff_t = abs(time2 - tt)
                tempn = np.argmin(diff_t)
                episode_steps.append(step_tuple[tempn])
        readf.write_to_file(pp_file, 'end_time', end_time, 'float')
        readf.write_to_file(pp_file, 'end_c_percent', end_c_percent, 'float')
        readf.write_to_file(pp_file, 'episode_completness',
                            episode_completness, 'float', 'array')
        readf.write_to_file(pp_file, 'episode_steps', episode_steps, 'int',
                            'array')
    else:
        plt.show()
    plt.close(fig)
Beispiel #14
0
def horiz_avg_1(in_dict, time_array, step_tuple, column_dict, route, o_dir,
                case_name):
    #plot horizontal_averagye result, no chemical
    nprocz = readf.get_variable(in_dict, 'nprocz', 'int')
    noz = readf.get_variable(in_dict, 'nodez', 'int')
    Ra = readf.get_variable(in_dict, 'rayleigh', 'float')
    Buoy = readf.get_variable(in_dict, 'buoyancy_ratio', 'float_list')
    Alpha = readf.get_variable(in_dict, 'thermexp', 'float')
    Tref = readf.get_variable(in_dict, 'reftemperature', 'float')
    Tsurf = readf.get_variable(in_dict, 'surftemperature', 'float')
    Rho = readf.get_variable(in_dict, 'density', 'float')
    Eta = readf.get_variable(in_dict, 'refvisc', 'float')
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    lnoz = int((noz - 1) / nprocz) + 1
    cols = column_dict['cols']
    n_c = len(column_dict['chemical'])
    #----derive scalings----#
    year = 365 * 24 * 3600
    r_scaling = Ro / 1e3
    time_scaling = pow(Ro, 2.0) / Kappa / (1e6 * year)
    velo_scaling = Kappa / Ro * year * 1e2
    #---output informations---#
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    temp_dir = Mpf.assign_output_dir("%s/temp" % (case_dir))
    velo_dir = Mpf.assign_output_dir("%s/velo" % (case_dir))
    visc_dir = Mpf.assign_output_dir("%s/visc" % (case_dir))
    for step in step_tuple:
        print(step, end='\r')
        data_in = readf.read_horig_output(route, case_name, step, nprocz, lnoz,
                                          cols)
        time = time_array[step] * time_scaling
        ##----plot figures----#
        col_r = column_dict['radius']
        ydata = data_in[:, col_r]
        settings = {
            'name': 'temp',
            'x_unit': '1',
            'y_unit': '1',
            'o_dir': temp_dir,
            'plot_type': 'n',
            'color': 'r',
            'mark': '.'
        }
        col_t = column_dict['temp']
        xdata = data_in[:, col_t]
        Mpf.plot_horiz_avg(xdata, ydata, step, time, settings)
        settings = {
            'name': 'visc',
            'x_unit': '1',
            'y_unit': '1',
            'o_dir': visc_dir,
            'plot_type': 'l',
            'color': 'b',
            'mark': '.'
        }
        col_v = column_dict['visc']
        xdata = data_in[:, col_v]
        Mpf.plot_horiz_avg(xdata, ydata, step, time, settings)
        settings = {
            'name': ['velo', 'vr', 'vth'],
            'x_unit': 'cm/yr',
            'y_unit': '1.0',
            'o_dir': velo_dir,
            'plot_type': 'n',
            'color': ('c', 'g'),
            'mark': '.'
        }
        xdata = np.zeros((noz, 2))
        col_vr = column_dict['vr']
        col_vth = column_dict['vth']
        xdata[:, 0] = data_in[:, col_vr]
        xdata[:, 1] = data_in[:, col_vth]
        Mpf.plot_horiz_avg(xdata, ydata, step, time, settings)
Beispiel #15
0
def plot_combine(in_dict, oroute, cname, dfile, tp, cdict, tval, **kwarg):
    def _config(name, default):
        try:
            return kwarg[name]
        except KeyError:
            return default

    dcwd = './gmt'
    Ro = readf.get_variable(in_dict, 'radius', 'float')
    Kappa = readf.get_variable(in_dict, 'thermdiff', 'float')
    ri = readf.get_variable(in_dict, 'radius_inner', 'float')
    Buoy = readf.get_variable(in_dict, 'buoyancy_ratio', 'float')
    Alpha = readf.get_variable(in_dict, 'thermexp', 'float')
    year = 365 * 24 * 3600
    Time = Ro**2.0 / Kappa / (1e6 * year)
    R = Ro / 1e5
    Temp = readf.get_variable(in_dict, 'reftemperature', 'float')
    Toff = readf.get_variable(in_dict, 'surftemperature', 'float')
    Tab = 273.15
    Toff = Toff - Tab
    Rho = readf.get_variable(in_dict, 'density', 'float')
    Drho = Buoy * Alpha * Temp * Rho
    tmin = tval[0]
    tmax = tval[1]
    tminor = tval[2]
    tmini = tval[3]
    rmin = R * ri
    rmax = R
    odir0 = Mpf.assign_output_dir('%s/%s' % (oroute, cname))
    odir = Mpf.assign_output_dir('%s/combine' % (odir0))
    ofile = '%s/combine_%s_%.0f_%.0f.ps' % (odir, tp, tmin, tmax)
    if tp is 'rho':
        Dat = Drho
        Doff = Rho
        dmin = Rho
        dmax = Rho + Drho
        dminor = _config('rhodminor', 5.0)
        coff = _config('rhocoff', 50.0)
    elif tp is 'temp':
        Dat = Temp
        Doff = Toff
        dmin = Toff
        dmax = Toff + Temp
        dminor = 50.0
        coff = 500.0
    t = cdict['time']
    r = cdict['radius']
    dat = cdict[tp]
    abash = []
    abash.append(
        'gmt nearneighbor -i%d[s%.4f],%d[s%.4f],%d[s%.4fo%.4f] -R%.4f/%.4f/%.4f/%.4f -I0.1/0.1 -S30 -N1 -Gresult.grd -V %s'
        % (t, Time, r, R, dat, Dat, Doff, tmin, tmax, rmin, rmax, dfile))
    cpt = _config('cpt', None)
    if cpt is None:
        abash.append('gmt makecpt -Cno_green -T%.4f/%.4f/%.4f > color.cpt' %
                     (dmin, dmax, dminor))
        cfile = 'color.cpt'
    else:
        cfile = cpt
    abash.append(
        'gmt grdimage result.grd -R%.4f/%.4f/%.4f/%.4f -C%s -JX4i/4i -Ba%.4ff%.4f:Time/Ma:/a4.0f2.0:Radius/100km:WSen -K -P > %s'
        % (tmin, tmax, rmin, rmax, cfile, tminor, tmini, ofile))
    abash.append(
        'gmt psscale -C%s -D4.4i/2.0i/4.0i/0.2i -P -O -V -B%.4f >> %s' %
        (cfile, coff, ofile))
    abash.append('gmt psconvert -A -Tj %s' % ofile)
    print(abash)  #debug
    readf.run_bash(abash, dcwd)
Beispiel #16
0
PVarray.append('cslice2')
PVarray.append('melting')
#image types from matlab goes here
MLarray.append('temp')
MLarray.append('rho')
MLarray.append('visc')
MLarray.append('velo')
include_field = 1
#image that is singular (not base on step) goes here
SGarray.append('chemical/overturned_IBC')
SGarray.append('chemical/retained_ibc')
SGarray.append('heat_flux/cmb_heatflux')
SGarray.append('vol/volume_value')
#steps of interest
steparray.append(0)
e_steps = Mread.get_variable(pp_dict, 'episode_steps', 'int_list')
for step in e_steps:
    if step > 0:
        steparray.append(step)
try:
    rsteps = Mread.get_variable(pp_dict, 'steps_remain', 'int_list')
except KeyError:
    map_to_index = 1
else:
    map_to_index = 0
    steparray.append(rsteps[-1])

picN = 0
fileO = '%s/summury.jpg' % (route)
maxStepPv = 100000  # max step for searching exitsting output file from CitcomS
#----map step to index of 3d figures----#
Beispiel #17
0
plot_MF_surf(Route, CaseName, 7400, oroute)
input()
#--------------------remove files----------------------------#
settings = {'col': 10}
settings['column'] = {
    'step': 0,
    'temp': 1,
    'melting': [5, 6, 7, 8, 9]
}  #first in melting is total melting
settings['color'] = {'temp': 'r', 'melting': ['k', 'r', 'b', 'g', 'c']}
#settings={'col':6}
#settings['column']={'step':0,'temp':1,'melting':[5]} #first in melting is total melting
#settings['color']={'temp':'r','melting':['k']}
#pp.plot_volume_1(inD,time_array,Route,oroute,CaseName,settings)
p_dict = Mread.read_input(ppFile)
e_steps = Mread.get_variable(p_dict, 'episode_steps', 'int_list')
e_ends = e_steps[len(e_steps) - 1]
#try:
#    steps_remain=Mread.get_variable(p_dict,'steps_remain','int_list')
#except KeyError:
#    pp.remove_extra_file(Route,CaseName,inD,time_array,Steps,ppFile,plogfile)
#else:
#    steps_remain_end = steps_remain[len(steps_remain)-1]
#    if steps_remain_end != Steps[len(Steps)-1]:
#        pp.remove_extra_file1(Route,CaseName,inD,time_array,Steps,steps_remain_end,ppFile,plogfile)
#pp.sph_plot(inD,rr,Route,oroute,CaseName,ppFile,6000,'T')
#--------------------------sph file-------------------------#
for step in e_steps:
    #for step in steps_remain:
    pp.sph_plot(inD, rr, Route, oroute, CaseName, ppFile, step, 'T')
#step = steps_remain[-1]
Beispiel #18
0
def sph_plot(in_dict, rr, route, o_dir, case_name, pp_file, step, vtype='T'):
    print('plot sph expansion figures, step %d\n' % step)
    color_mini = 0.05
    r_minor = 4.0
    r_mini = 2.0
    gmt_dir = Mpf.assign_output_dir("./gmt")
    file_out = ('%s/%s.field.%d.dat' % (gmt_dir, case_name, step))
    case_dir = Mpf.assign_output_dir("%s/%s" % (o_dir, case_name))
    field_dir = Mpf.assign_output_dir('%s/field' % (case_dir))
    radius = readf.get_variable(in_dict, 'radius', 'float')
    rin = readf.get_variable(in_dict, 'radius_inner', 'float')
    nprocz = readf.get_variable(in_dict, 'nprocz', 'int')
    noz = readf.get_variable(in_dict, 'nodez', 'int')
    ll_max = readf.get_variable(in_dict, 'output_ll_max', 'int')

    ofile = '%s/%s_field_%s_%d.ps' % (field_dir, case_name, vtype, step)
    ofile1 = '%s/%s_field_%s_%dl.eps' % (field_dir, case_name, vtype, step)
    lnoz = int((noz - 1) / nprocz) + 1
    nn_max = int((ll_max + 1) * (ll_max + 2) / 2)
    boundary = np.zeros(noz)
    boundary[0] = 1
    boundary[noz - 1] = 1
    #----read in data from .field output----#
    data = readf.read_field(route, case_name, nprocz, noz, ll_max, step)
    #----output file for gmt plot----#
    sph_max = np.zeros(noz)
    fout = open(file_out, 'w')
    for nz in range(noz):
        temp = data[nz, 1:ll_max + 1]
        ll0 = np.argmax(temp) + 1
        if boundary[nz]:
            sph_max[nz] = 0.0
            temp = temp * 0.0
        else:
            sph_max[nz] = temp[ll0 - 1]
            temp = temp / sph_max[nz]
        for ll in range(1, ll_max + 1):
            fout.write('%.4e %d %.4e\n' % (rr[nz], ll, temp[ll - 1]))
    fout.close()
    #----plot spectrum output with gmt----#
    ro = radius / 1e5
    ri = radius * rin / 1e5
    fig, ax = plt.subplots()
    plt.plot(sph_max, rr * ro, 'b-')
    ax.set(xlabel='Amplitude [1.0]', ylabel='Radius [100km]')
    plt.xlim(0.0, )
    plt.ylim(ri, ro)
    #plt.show()
    fig.savefig(ofile1)
    plt.close(fig)
    bashcommand = []
    bashcommand.append(
        'gmt nearneighbor -i1,0[s%.1f],2 -R1/%d/%.1f/%.1f -I1.0/0.3 -S1 -N1 -G%s/result.grd -V %s'
        % (ro, ll_max, ri, ro, gmt_dir, file_out))
    bashcommand.append('gmt makecpt -Cno_green -T0/1/%.3f > %s/color.cpt' %
                       (color_mini, gmt_dir))
    bashcommand.append(
        'gmt grdimage %s/result.grd -R1/%d/%.1f/%.1f/ -C%s/color.cpt -JX6i/3i -X1.0i -Y2.0i -Ba5f1:Degree:/a%.1ff%.1f:Radius/100km:WSen -P -K > %s'
        % (gmt_dir, ll_max, ri, ro, gmt_dir, r_minor, r_mini, ofile))
    bashcommand.append(
        'gmt psscale -D3.5i/-0.75i/15.0c/0.5ch -C%s/color.cpt -P -O -U -V -B:Power:0.1f0.1WSne >> %s'
        % (gmt_dir, ofile))
    bashcommand.append('gmt psconvert -A -Tj %s' % ofile)
    #    bashcommand.append('gmt psconvert -A -Tf %s'%ofile)
    ofile2 = '%s/%s_field_%s_%d.jpg' % (field_dir, case_name, vtype, step)
    ofile3 = '%s/%s_field_%s_%dl.png' % (field_dir, case_name, vtype, step)
    bashcommand.append('convert %s -resize x1368 %s' % (ofile1, ofile3))
    bashcommand.append('convert %s %s +append %s' % (ofile2, ofile3, ofile2))
    #print(bashcommand) #debug
    #input()
    readf.run_bash(bashcommand)
    #os.remove(ofile1)
    os.remove(ofile3)