def test_ghost_zones():
ds = yt.load(output_00080)
def gen_dummy(ngz):
def dummy(field, data):
if not isinstance(data, FieldDetector):
shape = data["gas", "mach_number"].shape[:3]
np.testing.assert_equal(
shape, (2 + 2 * ngz, 2 + 2 * ngz, 2 + 2 * ngz))
return data["gas", "mach_number"]
return dummy
fields = []
for ngz in (1, 2, 3):
fname = ("gas", f"density_ghost_zone_{ngz}")
ds.add_field(
fname,
gen_dummy(ngz),
sampling_type="cell",
validators=[yt.ValidateSpatial(ghost_zones=ngz)],
)
fields.append(fname)
box = ds.box([0, 0, 0], [0.1, 0.1, 0.1])
for f in fields:
print("Getting ", f)
box[f]
### THIS RECIPE IS CURRENTLY BROKEN IN YT-3.0
### DO NOT TRUST THIS RECIPE UNTIL THIS LINE IS REMOVED
import numpy as np
import yt
# Define the components of the gravitational acceleration vector field by
# taking the gradient of the gravitational potential
@yt.derived_field(name='gravitational_acceleration_x',
units='cm/s**2', take_log=False,
validators=[yt.ValidateSpatial(1,["gravitational_potential"])])
def gravitational_acceleration_x(field, data):
# We need to set up stencils
sl_left = slice(None, -2, None)
sl_right = slice(2, None, None)
div_fac = 2.0
dx = div_fac * data['dx'][0]
gx = data["gravitational_potential"][sl_right, 1:-1, 1:-1]/dx
gx -= data["gravitational_potential"][sl_left, 1:-1, 1:-1]/dx
new_field = np.zeros(data["gravitational_potential"].shape,
dtype='float64')*gx.uq
new_field[1:-1, 1:-1, 1:-1] = -gx
return new_field
def rhologrho(field, data):
return data['Density'] * data['logrho']
def cs2rhologrho(field, data):
cs2 = data.ds.quan(1., 'code_velocity**2')
return cs2 * data['rhologrho']
def ek(field, data):
return 0.5 * data['Density'] * data['absv']**2
default_validators = [yt.ValidateGridType()]
density_validators = [yt.ValidateSpatial(1, ['density'])]
vx_validators = [yt.ValidateSpatial(1, ['x-velocity'])]
vy_validators = [yt.ValidateSpatial(1, ['y-velocity'])]
vz_validators = [yt.ValidateSpatial(1, ['z-velocity'])]
drho_units = "code_mass/code_length**4"
dv_units = "1/code_time"
a_units = "code_length/code_time**2"
fields = {
"drhodx": [drhodx, density_validators, drho_units, {}],
"drhody": [drhody, density_validators, drho_units, {}],
"drhodz": [drhodz, density_validators, drho_units, {}],
"absv": [absv, "code_length/code_time", {}],
"dvxdx": [dvxdx, vx_validators, dv_units, {}],
"dvxdy": [dvxdy, vx_validators, dv_units, {}],
#print " search"
found_any, mask = particle_ops.mask_particles(
indices_late, my_indices, mask_to_get)
data.set_field_parameter('mask_to_get',mask_to_get)
pos_to_get = data['particle_position'][mask == 1]
d = data.deposit(pos_to_get, method = "count")
d = data.ds.arr(d, input_units = "cm**-3")
t1 = time.time()
#print " DT", t1-t0[-1]
data.set_field_parameter('timer',t0+[t1])
return data.apply_units(d, field.units)
yt.add_field( ("deposit","deposit_target_particles"),
#yt.add_field( 'dp1',
function = deposit_target_particles_1,
validators = [yt.ValidateSpatial(),
yt.ValidateParameter('indices_late'),
yt.ValidateParameter('mask_to_get'),
yt.ValidateGridType()],
display_name = "target_particles")
class SelectParticleCallback(PlotCallback):
_type_name = "select_particles"
region = None
_descriptor = None
def __init__(self, width, p_size=1.0, col='k', marker='o', stride=1.0,
ptype='all', stars_only=False, dm_only=False,
minimum_mass=None,bool=None, indices=None, xyz=None):
"""
Adds particle positions, based on a thick slab along *axis* with a
*width* along the line of sight. *p_size* controls the number of
