예제 #1
0
plane.rectangle_e(center=[126,551], xlen=20, ylen=8,   value=1)


metal = PolarDPlane(plane.shape, a=(1.757*10**16)**2, b=0, c=3.0786*10**14, d=1, dt=plane.dt()).set_factor()
metal.rectangle(center=[151,351], xlen=70, ylen=710, value=1)
metal.rectangle(center=[151,351], xlen=70, ylen=8,   value=0)
metal.rectangle(center=[126,251], xlen=20, ylen=8,   value=0)
metal.rectangle(center=[126,451], xlen=20, ylen=8,   value=0)
metal.rectangle(center=[126,151], xlen=20, ylen=8,   value=0)
metal.rectangle(center=[126,551], xlen=20, ylen=8,   value=0)

dt = plane.dt()
freq = plane.frequency()

for t in range(0,7000):
    stdout.write("\b\b\b\b%d"%t)
    plane.t = t

    plane.teinc.update(cos(2*pi*freq*t*dt)*gaussian(t*dt, 800*dt, 150*dt))#.plot_e("result/grating-slit/teinc/teinc-%.4d.png"%t)

    plane.update_dfield().update_dtfsf()
    metal.update(plane)
    plane.update_efield(metal).update_epbc()

    plane.update_bfield().update_btfsf()
    plane.update_hfield().update_hpbc()

    plane.imshow_hz("result/grating-slit/hz/grating-slit-%.4d.png"%t)
    plane.save()

# metal = PolarDPlane(plane.shape, a=(9.39*10**15)**2, b=0, c=3.14*10**13, d=1, dt=plane.attrs["dt"])
metal = PolarDPlane(plane.shape, a=(1.757*10**16)**2, b=0, c=3.0786*10**14, d=1, dt=plane.attrs["dt"])
metal.set_factor()
metal.circle([151,151], 25)

prepare("result/%s/ex" % plane.name)
prepare("result/%s/ey" % plane.name)
prepare("result/%s/hz" % plane.name)

for t in range(0,4500):
    plane.t = t
    plane.teinc.update(sin(2*pi*plane.attrs["frequency"]*t*plane.attrs["dt"]))

    plane.update_hpbc()
    plane.update_dfield().update_dtfsf()
    metal.update(plane)
    plane.update_efield(metal)

    plane.update_epbc()
    plane.update_bfield().update_btfsf()
    plane.update_hfield()

    plane.save()
    plane.imshow_ex("result/%s/ex/%.4d.png" % (plane.name, t))
    plane.imshow_ey("result/%s/ey/%.4d.png" % (plane.name, t))
    plane.imshow_hz("result/%s/hz/%.4d.png" % (plane.name, t))
    print t

plane.close()