Example #1
0
def test02_roughconductor(variant_scalar_rgb):
    from mitsuba.core.xml import load_string
    from mitsuba.render import BSDF, BSDFContext, SurfaceInteraction3f
    from mitsuba.core import Frame3f

    for alpha in [(0.3, 0.3), (0.3 + 1e-5, 0.3 - 1e-5), (0.2, 0.4)]:
        alpha_u = alpha[0]
        alpha_v = alpha[1]

        thetas = np.linspace(0, np.pi / 2, 20)
        phi = np.pi

        values_ref = []

        # Create conductor reference BSDF
        bsdf = load_string("""<bsdf version="2.0.0" type="roughconductor">
                                  <float name="alpha_u" value="{}"/>
                                  <float name="alpha_v" value="{}"/>
                                  <string name="distribution" value="beckmann"/>
                                  <spectrum name="eta" value="0.0"/>
                                  <spectrum name="k" value="1.0"/>
                              </bsdf>""".format(alpha_u, alpha_v))

        theta_i = np.radians(30.0)
        si = SurfaceInteraction3f()
        si.p = [0, 0, 0]
        si.n = [0, 0, 1]
        si.wi = [np.sin(theta_i), 0, np.cos(theta_i)]
        si.sh_frame = Frame3f(si.n)
        ctx = BSDFContext()

        for theta in thetas:
            wo = [
                np.sin(theta) * np.cos(phi),
                np.sin(theta) * np.sin(phi),
                np.cos(theta)
            ]
            values_ref.append(bsdf.eval(ctx, si, wo=wo)[0])

        # Create same BSDF as layer representation
        n, ms, md = mitsuba.layer.microfacet_parameter_heuristic(
            alpha_u, alpha_v, 0 + 1j)
        mu, w = mitsuba.core.quad.gauss_lobatto(n)
        layer = mitsuba.layer.Layer(mu, w, ms, md)
        layer.set_microfacet(0 + 1j, alpha_u, alpha_v)

        for i, theta in enumerate(thetas):
            l_eval = layer.eval(-np.cos(theta), np.cos(theta_i)) * np.abs(
                np.cos(theta))
            # Values should be close (except if they are insignificantly small).
            # We have less precision at grazing angles because of Fourier representation.
            print(values_ref[i], l_eval)
            assert values_ref[i] < 1e-5 or np.allclose(
                values_ref[i], l_eval, rtol=0.05 / (np.abs(np.cos(theta))))

        # Convert into BSDF storage representation
        base_path = os.path.dirname(os.path.realpath(__file__)) + "/data/"
        if not os.path.exists(base_path):
            os.makedirs(base_path)
        path = base_path + "roughconductor.bsdf"
        storage = mitsuba.layer.BSDFStorage.from_layer(path, layer, 1e-8)

        for i, theta in enumerate(thetas):
            s_eval = storage.eval(np.cos(theta_i), -np.cos(theta))[0]
            # Values should be close (except if they are insignificantly small).
            # We have less precision at grazing angles because of Fourier representation.
            assert values_ref[i] < 1e-5 or np.allclose(
                values_ref[i], s_eval, rtol=0.05 / (np.abs(np.cos(theta))))
        storage.close()

        # And load via the "fourier" BSDF plugin
        fourier = load_string("""<bsdf version="2.0.0" type="fourier">
                                     <string name="filename" value="{}"/>
                                 </bsdf>""".format(path))

        for i, theta in enumerate(thetas):
            wo = [
                np.sin(theta) * np.cos(phi),
                np.sin(theta) * np.sin(phi),
                np.cos(theta)
            ]
            f_eval = fourier.eval(ctx, si, wo=wo)[0]
            assert values_ref[i] < 1e-5 or np.allclose(
                values_ref[i], f_eval, rtol=0.05 / (np.abs(np.cos(theta))))
        del fourier
Example #2
0
alpha_v = 0.2
eta = 0+1j

n, ms, md = mitsuba.layer.microfacet_parameter_heuristic(alpha_u, alpha_v, eta)
mu, w = mitsuba.core.quad.gauss_lobatto(n)
print(n, ms, md)
print("")

for s in [1, 3, 9]:
    if s > ms:
        break

    print('ms: ', s)

    layer = mitsuba.layer.Layer(mu, w, s, md)
    layer.set_microfacet(eta, alpha_u, alpha_v)
    layer.clear_backside()

    filename = "%.02f_%.02f_%02d.bsdf" % (alpha_u, alpha_v, s)
    storage = mitsuba.layer.BSDFStorage.from_layer(filename, layer, 1e-8)


# Example 2: Extreme anisotropy

alpha_u = 0.05
alpha_v = 0.4
eta = 0+1j

n, ms, md = mitsuba.layer.microfacet_parameter_heuristic(alpha_u, alpha_v, eta)
mu, w = mitsuba.core.quad.gauss_lobatto(n)
print(n, ms, md)
Example #3
0
    n1, ms1, md1 = mitsuba.layer.microfacet_parameter_heuristic(
        alpha_u_top, alpha_v_top, eta_top)
    n2, ms2, md2 = mitsuba.layer.microfacet_parameter_heuristic(
        alpha_u_bot, alpha_v_bot, eta_bot[0])
    n = max(n1, n2)
    ms = max(ms1, ms2)
    md = md2
    mu, w = mitsuba.core.quad.gauss_lobatto(n)

    print("   dielectric top")
    dielectric = mitsuba.layer.Layer(mu, w, ms, md)
    dielectric.set_microfacet(eta_top, alpha_u_top, alpha_v_top)

    channels = []
    for i in range(3):
        print("   gold base [%d]" % i)
        layer = mitsuba.layer.Layer(mu, w, ms, md)
        layer.set_microfacet(eta_bot[i], alpha_u_bot, alpha_v_bot)
        layer.clear_backside()

        layer.add_to_top(dielectric, epsilon=1e-6)

        channels.append(layer)

        print("    save")
    filename = "%s.bsdf" % key
    storage = mitsuba.layer.BSDFStorage.from_layer_rgb(filename, *channels, 1,
                                                       1e-4)

    print("\n")