def setUp(self):
self.wp = Waveplate(direction=(0.,0.,1.))
self.src = ParallelRaySource(rings=0,
E_vector=(1,0,0),
E1_amp = 1.0+0.0j,
E2_amp = 0.0+0.0j,
direction = (0,0,1),
origin = (0,0,-10),
)
self.model = RayTraceModel(optics=[self.wp,],
sources=[self.src])
def test_quarter_retardance2(self):
src = SingleRaySource(E_vector=(1,0,0),
E1_amp = 1.0+0.0j,
E2_amp = 0.0+0.0j,
direction = (0,0,1),
origin = (0,0,-40),
)
wp1 = Waveplate(retardance=0.25,
rotation = 45.0,
centre=(0,0,40),
direction=(0,0,1))
print("wp1 fa:", wp1.material.fast_axis)
wp2 = Waveplate(retardance=0.25,
rotation = -45.0,
centre=(0,0,80),
direction=(0,0,-1))
print("wp2 fa:", wp2.material.fast_axis)
print("wp1 fa:", wp1.material.fast_axis)
model = RayTraceModel(optics=[wp1,wp2], sources=[src])
model.trace_all()
def get_major_axis(ray):
E1_vector = numpy.array(ray.E_vector)
E2_vector = numpy.cross(numpy.array(ray.direction),
E1_vector)
E = (E1_vector*ray.E1_amp + E2_vector*ray.E2_amp)
return E.real
ray_in = src.InputRays[0]
#print ray_in.E_vector, ray_in.E1_amp, ray_in.E2_amp
self.assertEqual(len(src.TracedRays), 3)
for i in range(len(src.TracedRays)):
ray = src.TracedRays[i][0]
print(i, "::", get_major_axis(ray), ray.E_left, ray.E_right, ray.ellipticity, ray.E_vector)
def test_quarter_retardance(self):
src = SingleRaySource(E_vector=(1,0,0),
E1_amp = 1.0+0.0j,
E2_amp = 0.0+0.0j,
direction = (0,0,1),
origin = (0,0,-40),
)
wp = Waveplate(retardance=0.25,
rotation = 45.0,
centre=(0,0,40),
direction=(0,0,1))
m = PECMirror(centre=(0,0,80),
direction=(0.0,0.0,1.0))
model = RayTraceModel(optics=[wp,m], sources=[src])
#model.trace_all()
def get_major_axis(ray):
E1_vector = numpy.array(ray.E_vector)
E2_vector = numpy.cross(numpy.array(ray.direction),E1_vector
)
E = (E1_vector*ray.E1_amp + E2_vector*ray.E2_amp)
return E
ray_in = src.InputRays[0]
#print ray_in.E_vector, ray_in.E1_amp, ray_in.E2_amp
self.assertEqual(len(src.TracedRays), 4)
for i in range(4):
ray = src.TracedRays[i][0]
print(i, "::", ray.E_left, ray.E_right, ray.E_vector, ray.E1_amp, ray.E2_amp)
print("\t", get_major_axis(ray))
ray_out = src.TracedRays[-1][0]
self.assertAlmostEqual(numpy.dot(get_major_axis(ray_out),
get_major_axis(ray_in)), 0.0)
sys.path.append('..')
import pyximport
pyximport.install()
from raytrace.tracer import RayTraceModel
from raytrace.sources import BroadbandRaySource
from raytrace.diffraction_gratings import RectangularGrating
source = BroadbandRaySource(number=5,
wavelength_start=1.5,
wavelength_end=1.6,
uniform_deltaf=True,
origin=(-50, 0, 0),
direction=(1., 0, 0))
grating = RectangularGrating(length=25.4,
width=25.4,
thickness=6.0,
centre=(0.0, 0.0, 0.0),
direction=(-1, 0, 0),
lines_per_mm=600,
efficiency=1.0,
order=1)
rays = source.InputRays
model = RayTraceModel(optics=[grating], sources=[
source,
])
model.configure_traits()
D2 = np.dot(rot_matrix,D2)-trans_vector
c21 = np.dot(rot_matrix,c21)-trans_vector
c22 = np.dot(rot_matrix,c22)-trans_vector
E2 = np.dot(rot_matrix,E2)-trans_vector
left_arm = Extruded_bezier(name = "left arm",control_points = np.array([[D2,c21,c22,E2]]),z_height_1 = 0, z_height_2 = system_length, material = PECMaterial())
target = RectTarget(width = len_exit_ap, length = system_length, elevation=90., rotation =90., centre = (0,0,system_length/2.))
source = RectRaySource(origin=(0,100,system_length/4.),
direction=(0,-1,0),
working_dist = 200.,
number=10,
length = system_length/4.,
width = 10, #lea+2*E[0],
randomness = True,
theta = 10.00000001)
raypaths = RayPaths()
model = RayTraceModel(sources=[source],
optics=[target, right_arm,left_arm], results = [raypaths], recursion_limit=10)
model.configure_traits()
profile[len(profile):] = xtr_pts
self.profile = profile
#print profile
#polygon approximation of parabolic trough mirror
para = approx_parabola(material=PECMaterial(),
z_height_1=-20.0,
z_height_2=20.0,
focal_length=10)
print(0)
model0 = RayTraceModel(optics=[
para,
], sources=[
source,
])
print(1)
model1 = RayTraceModel(optics=[
para,
], sources=[
source,
])
print(2)
model2 = RayTraceModel(optics=[
para,
], sources=[
source,
])
print(3)
randomness=True)
#linear dialectric filled light funnel
r1 = LDLF( #material=OpaqueMaterial(),
z_height_1=-20.0,
z_height_2=20.0,
slat_width=slat_width,
ap_width=ex_ap,
slant=slant,
n_inside=1.333) #1.333 = water
ratio = Ratio(denominator=r1.faces[2], nominator=r1.faces[0])
raypaths = RayPaths()
model = RayTraceModel(optics=[
r1,
],
sources=[s1, s2, s3, s4, s5],
results=[ratio, raypaths],
recursion_limit=5)
entry_ap = r1.faces.faces[2]
newsource = trace_pretty(model, 1, [entry_ap])
model.sources = [
newsource,
]
#model.configure_traits()
#print model.all_faces
#ap_ratio = ent_ap/ex_ap
#print "ap ratio: ", ap_ratio
#print "effective concentration: ", ap_ratio*model.results[0].result #still not right, circular source biases ratio.
from raytrace.tracer import RayTraceModel
from raytrace.parabolics import OffAxisParabloid
from raytrace.sources import ConfocalRaySource
h = 25.4
oap = OffAxisParabloid(diameter=50.4, height=h, EFL=50.4)
source = ConfocalRaySource(focus=(0, 0, 0),
direction=(1, 0, 0),
working_dist=10.0,
number=8,
rings=2,
theta=15.0,
export_pipes=True)
model = RayTraceModel(optics=[oap], sources=[source])
model.configure_traits()
show_polarisation: false
show_start: true
- !SolidRetroreflector
__traits_version__: 3.3.0
_orientation: !!python/tuple [0.0, 0.0]
all_rays: false
centre: !!python/tuple [0.0, 0.0, 0.0]
diameter: 25.399999999999999
direction: !!python/tuple [0.0, 0.0, 1.0]
display: shaded
elevation: 0.0
material: !!python/object:raytrace.cmaterials.DielectricMaterial {}
n_inside: !!python/complex '1.5'
n_outside: !!python/complex '1.0'
name: Solid Retroreflector
orientation: 0.0
rotation: 0.0
thickness: 20.0
"""
import yaml
print(yaml.dump([source, cc]))
source, cc = yaml.load(data)
model = RayTraceModel(sources=[source], optics=[cc])
model.configure_traits()
#model.update = True
#print source.TracedRays
source = ParallelRaySource(
origin=(0, 20, 0),
direction=(0, -1, 1),
working_dist=10.,
#number=20,
radius=1.)
#print source.InputDetailRays.origin.shape
m1 = TroughParabloid(width=20, length=100, EFL=5, centre=(0, 0, 0))
print(m1.intersect)
model = RayTraceModel(optics=[
m1,
],
sources=[
source,
],
probes=[],
recursion_limit=2)
#model.trace_detail_async()
#import time
#start = time.clock()
#model.trace_all()
#end = time.clock()
#print "traced in", end - start
model.configure_traits()
working_dist=100.,
number=4,
rings=1,
detail_resolution=5,
theta=10.)
w1 = PlanarWindow(diameter=25.4,
thickness=5.0,
centre=(0, -20, 0),
direction=(0, 1, 1),
n_inside=3.4,
name="w1")
model = RayTraceModel(optics=[
w1,
], sources=[
source,
])
#model.trace_detail_async()
#import time
#start = time.clock()
#model.trace_all()
#end = time.clock()
#print "traced in", end - start
#import timeit
#t = timeit.Timer("model.update = True","from __main__ import model")
#ret = t.timeit(10)
#print "time:", ret
from raytrace.results import Ratio
import numpy
source = ConfocalRaySource(focus=(0,0,0),
direction=(0,1,0),
working_dist = 100.,
number=20,
detail_resolution=5,
theta=10.)
#print source.InputDetailRays.origin.shape
m1 = PECMirror(name="M1",
centre=(0,-40,0),
direction=(0,1,-1),
diameter=30.,
thickness=5.)
l1 = PlanoConvexLens(centre=(0,-40,30),
direction=(0,0,1))
ratio = Ratio(denominator=m1.faces[0],
nominator=l1.faces[1])
model = RayTraceModel(optics=[m1,l1],
sources=[source,],
results=[ratio])
model.configure_traits()
source = RectRaySource(origin=(10, 30, 0),
direction=(.1, -1, 0),
working_dist=100.,
number=1,
length=0,
width=0,
randomness=False,
scale_factor=0.2)
'''
source = RectRaySource(origin=(10.,10.,0),
direction=(.2,-1,0),
working_dist = 100.,
number=3,
length = 12,
width = 12,
randomness = False,
scale_factor=0.2)
'''
raypaths = RayPaths()
model = RayTraceModel(sources=[source],
optics=[test],
results=[raypaths],
recursion_limit=10)
#test.invert_normal = True
hits = model.sources[0].TracedRays
res = model.results[0].result
model.configure_traits()
e1 = Ellipsoid(focus1=(0,-40,40),
focus2=(0,0,80),
size=80,
X_bounds=(-30,0),
Y_bounds=(-15,15),
Z_bounds=(40-15.,40+15.))
e2 = Ellipsoid(focus1=(0,40,40),
focus2=(0,0,80),
size=80,
X_bounds=(0,30),
Y_bounds=(-15,15),
Z_bounds=(40-15.,40+15.))
l1 = PlanoConvexLens(centre=(0,-40,30),
direction=(0,0,1))
model = RayTraceModel(optics=[m1,m2,m3,m4,m5,e1,e2, l1],
sources=[source,],
probes=[p1,])
#model.trace_detail_async()
#import time
#start = time.clock()
#model.trace_all()
#end = time.clock()
#print "traced in", end - start
model.configure_traits()
from raytrace.tracer import RayTraceModel
from raytrace.lenses import PlanoConvexLens
from raytrace.sources import ConfocalRaySource
lens = PlanoConvexLens(centre=(20, 0, 0),
direction=(1, 0, 0),
curvature=25.0,
diameter=25.4,
CT=6.0)
source = ConfocalRaySource(focus=(0, 0, 0),
direction=(1, 0, 0),
working_dist=100.0,
theta=15.0)
model = RayTraceModel(optics=[lens], sources=[source])
model.configure_traits()
#try to make s as small as possible without making too many faces. (20 faces isn't unreasonable)
test = Extruded_interpolant(profile = [xs,ys], smoothness = 0, z_height_1 = -30, z_height_2=30, \
material = DielectricMaterial(), n_inside=1.5, trace_ends= True,trace_top = False )
source = RectRaySource(origin=(50,0,0),
direction=(-1,0,0),
working_dist = 100.,
number=10,
length = 10,
width = 10,
randomness = True,
theta = 5.,
scale_factor=0.2)
'''
r1 = LDLF(material=PECMaterial(),
z_height_1=-20.0,
z_height_2=20.0,
slat_width=20,
ap_width=5,
slant=75,
n_inside=1.7)
'''
model = RayTraceModel(sources=[source],
optics=[test])
model.configure_traits()
for i, center in enumerate(centers):
Mirrors[i] = RectMirror(width=mirror_width,
length=300.,
direction=(center, numpy.tan(-phi[i]) * center, 0),
centre=(center, 0, 0))
Optics = Mirrors
sorber = RectAbsorber(width=mirror_width,
length=300.,
direction=(0, -1, 0),
centre=(0, tower_height, 0))
Optics.append(sorber)
model = RayTraceModel(
sources=[
sun,
],
optics=Optics,
)
#model.trace_detail_async()
#import time
#start = time.clock()
#model.trace_all()
#end = time.clock()
#print "traced in", end - start
model.configure_traits()
y1=height_offset,
x2=-ent_ap / 2,
y2=height_offset,
z_height_1=0,
z_height_2=30,
material=TransparentMaterial())
exit_ap = Sheet(x1=ex_ap / 2,
y1=0,
x2=-ex_ap / 2,
y2=0,
z_height_1=0,
z_height_2=30,
material=TransparentMaterial())
ratio = Ratio(denominator=en_ap.faces[0], nominator=exit_ap.faces[0])
model = RayTraceModel(optics=[r1, r2, en_ap, exit_ap],
sources=[
source,
],
results=[ratio])
model.configure_traits()
print(model.all_faces)
ap_ratio = ent_ap / ex_ap
print("ap ratio: ", ap_ratio)
print("effective concentration: ", ap_ratio *
model.results[0].result) #still not right, circular source biases ratio.
#number=20,
radius=14.)
"""
s2 = ParallelRaySource(origin=(x,y,z),
direction=(xd,yd,zd),
working_dist = 50.,
#number=20,
radius=0)
"""
#print source.InputDetailRays.origin.shape
m1 = CylindricalInvolute(width = 60,
length = 500,
tube_radius = 5,
begin_angle = -90.,
end_angle = 500.)
model = RayTraceModel(optics=[m1,],
sources=[s1,],
probes=[])
#model.trace_detail_async()
#import time
#start = time.clock()
#model.trace_all()
#end = time.clock()
#print "traced in", end - start
model.configure_traits()
from raytrace.tracer import RayTraceModel model = RayTraceModel() model.configure_traits()
#print source.InputDetailRays.origin.shape
m1 = PECMirror(name="M1",
centre=(0,-40,0),
direction=(0,1,-1),
diameter=30.,
thickness=5.)
aligned = RectAperture(name="entry",
centre = (0,5,15),
direction = (0,1,0),
length = 30.,
width = 30.)
antialigned = RectAperture(name="reversed",
centre = (0,-5,15),
direction = (0,-1,0),
length = 30.,
width = 30.)
l1 = PlanoConvexLens(centre=(0,-40,30),
direction=(0,0,1))
ratio = Total_Efficency(Target=m1.faces[0],
Aperture=aligned.faces[0])
model = RayTraceModel(optics=[m1,aligned,antialigned],
sources=[source,],
results=[ratio])
model.configure_traits()
z_height_1=-20.0,
z_height_2=20.0,
slat_width=5.0, #
ap_width=3.0,
slant=80.0,
n_inside=3) #1.5 = glass, 3 = something crazy
class Ap_match_Constraint(BaseConstraint):
r1 = Instance(LDLF, ())
r2 = Instance(LDLF, ())
@on_trait_change("r1.update")
def calc_r2_param(self):
h = self.r1.slat_width / numpy.sin(self.r1.slant * numpy.pi / 180.)
self.r2.centre = (0, h, 0)
x = self.r1.ap_width + 2 * self.r1.slat_width * numpy.cos(
self.r1.slant * numpy.pi / 180.)
self.r2.ap_width = x
c = Ap_match_Constraint(r1=r1, r2=r2)
model = RayTraceModel(optics=[r1, r2], constraints=[
c,
], sources=[
source,
])
model.configure_traits()