Repository: karllark/dust_extinction

Issue:
Add in WD01 non-MW models

Discussion:

Patch:
diff --git a/docs/dust_extinction/choose_model.rst b/docs/dust_extinction/choose_model.rst
index 523e088..01044c4 100644
--- a/docs/dust_extinction/choose_model.rst
+++ b/docs/dust_extinction/choose_model.rst
@@ -148,11 +148,23 @@ observationally (e.g., in the extreme UV below 912 A).
 | Model        |    x range     | wavelength range |       galaxy |
 |              |    [1/micron]  | [micron]         |              |
 +==============+================+==================+==============+
-| D03_MWRV31   | 0.0001 - 10000 |   0.0001 - 10000 |           MW |
+| WD01 MWRV31  |   0.0001 - 100 |     0.01 - 10000 |  MW R(V)=3.1 |
 +--------------+----------------+------------------+--------------+
-| D03_MWRV40   | 0.0001 - 10000 |   0.0001 - 10000 |           MW |
+| WD01 MWRV40  |   0.0001 - 100 |     0.01 - 10000 |  MW R(V)=4.0 |
 +--------------+----------------+------------------+--------------+
-| D03_MWRV55   | 0.0001 - 10000 |   0.0001 - 10000 |           MW |
+| WD01 MWRV55  |   0.0001 - 100 |     0.01 - 10000 |  MW R(V)=5.5 |
 +--------------+----------------+------------------+--------------+
-| ZDA04_MWRV55 |  0.0001 - 1000 |    0.001 - 10000 |           MW |
+| WD01 LMCAvg  |   0.0001 - 100 |     0.01 - 10000 |          LMC |
++--------------+----------------+------------------+--------------+
+| WD01 LMC2    |   0.0001 - 100 |     0.01 - 10000 |  LMC2 Region |
++--------------+----------------+------------------+--------------+
+| WD01 SMCBar  |   0.0001 - 100 |     0.01 - 10000 |          SMC |
++--------------+----------------+------------------+--------------+
+| D03 MWRV31   | 0.0001 - 10000 |   0.0001 - 10000 |  MW R(V)=3.1 |
++--------------+----------------+------------------+--------------+
+| D03 MWRV40   | 0.0001 - 10000 |   0.0001 - 10000 |  MW R(V)=4.0 |
++--------------+----------------+------------------+--------------+
+| D03 MWRV55   | 0.0001 - 10000 |   0.0001 - 10000 |  MW R(V)=5.5 |
++--------------+----------------+------------------+--------------+
+| ZDA04 MWRV31 |  0.0001 - 1000 |    0.001 - 10000 |           MW |
 +--------------+----------------+------------------+--------------+
diff --git a/docs/dust_extinction/model_flavors.rst b/docs/dust_extinction/model_flavors.rst
index 6ab90e0..d2e9148 100644
--- a/docs/dust_extinction/model_flavors.rst
+++ b/docs/dust_extinction/model_flavors.rst
@@ -282,6 +282,99 @@ R(V) (+ other variables) dependent prediction models
    plt.show()
 
 
+Grain models
+============
+
+   These models provide literature grain models
+   interpolated between the computed data points.
+   These dust grain models are based on fitting observed extinction curves and
+   other observed properties of dust (e.g., abundances, IR emission).
+   Models are provided for the Milky Way calculated for the X-ray to the submm.
+
+.. plot::
+
+   import numpy as np
+   import matplotlib.pyplot as plt
+   import astropy.units as u
+
+   from dust_extinction.grain_models import WD01, D03, ZDA04
+
+   fig, ax = plt.subplots()
+
+   # generate the curves and plot them
+   lam = np.logspace(-4.0, 4.0, num=1000)
+   x = (1.0 / lam) / u.micron
+
+   models = [WD01, WD01, WD01,
+             D03, D03, D03,
+             ZDA04]
+   modelnames = ["MWRV31", "MWRV40", "MWRV55",
+                 "MWRV31", "MWRV40", "MWRV55",
+                 "BARE-GR-S"]
+
+   for cmodel, cname in zip(models, modelnames):
+      ext_model = cmodel(cname)
+
+      indxs, = np.where(np.logical_and(
+         x.value >= ext_model.x_range[0],
+         x.value <= ext_model.x_range[1]))
+      yvals = ext_model(x[indxs])
+      ax.plot(lam[indxs], yvals, label=f"{ext_model.__class__.__name__}  {cname}")
+
+   ax.set_xlabel('$\lambda$ [$\mu m$]')
+   ax.set_ylabel('$A(x)/A(V)$')
+   ax.set_title('Grain Models')
+
+   ax.set_xscale('log')
+   ax.set_yscale('log')
+
+   ax.set_title('Milky Way')
+
+   ax.legend(loc='best')
+   plt.tight_layout()
+   plt.show()
+
+
+.. plot::
+
+  import numpy as np
+  import matplotlib.pyplot as plt
+  import astropy.units as u
+
+  from dust_extinction.grain_models import WD01
+
+  fig, ax = plt.subplots()
+
+  # generate the curves and plot them
+  lam = np.logspace(-4.0, 4.0, num=1000)
+  x = (1.0 / lam) / u.micron
+
+  models = [WD01, WD01, WD01]
+  modelnames = ["LMCAvg", "LMC2", "SMCBar"]
+
+  for cmodel, cname in zip(models, modelnames):
+     ext_model = cmodel(cname)
+
+     indxs, = np.where(np.logical_and(
+        x.value >= ext_model.x_range[0],
+        x.value <= ext_model.x_range[1]))
+     yvals = ext_model(x[indxs])
+     ax.plot(lam[indxs], yvals, label=f"{ext_model.__class__.__name__}  {cname}")
+
+  ax.set_xlabel('$\lambda$ [$\mu m$]')
+  ax.set_ylabel('$A(x)/A(V)$')
+  ax.set_title('Grain Models')
+
+  ax.set_xscale('log')
+  ax.set_yscale('log')
+
+  ax.set_title('LMC & SMC')
+
+  ax.legend(loc='best')
+  plt.tight_layout()
+  plt.show()
+
+
 Shape fitting models
 ====================
 
@@ -379,48 +472,3 @@ Shape fitting models
    ax.legend(loc='best')
    plt.tight_layout()
    plt.show()
-
-Grain models
-==============
-
-   These models provide literature grain models
-   interpolated between the computed data points.
-   These dust grain models are based on fitting observed extinction curves and
-   other observed properties of dust (e.g., abundances, IR emission).
-   Models are provided for the Milky Way calculated for the X-ray to the submm.
-
-.. plot::
-
-   import numpy as np
-   import matplotlib.pyplot as plt
-   import astropy.units as u
-
-   from dust_extinction.grain_models import (D03_MWRV31, D03_MWRV40, D03_MWRV55,
-                                             ZDA04_MWRV31)
-
-   fig, ax = plt.subplots()
-
-   # generate the curves and plot them
-   lam = np.logspace(-4.0, 4.0, num=1000)
-   x = (1.0 / lam) / u.micron
-
-   models = [D03_MWRV31, D03_MWRV40, D03_MWRV55, ZDA04_MWRV31]
-
-   for cmodel in models:
-      ext_model = cmodel()
-      indxs, = np.where(np.logical_and(
-         x.value >= ext_model.x_range[0],
-         x.value <= ext_model.x_range[1]))
-      yvals = ext_model(x[indxs])
-      ax.plot(1.0/x[indxs], yvals, label=ext_model.__class__.__name__)
-
-   ax.set_xlabel('$\lambda$ [$\mu m$]')
-   ax.set_ylabel('$A(x)/A(V)$')
-   ax.set_title('Grain Models')
-
-   ax.set_xscale('log')
-   ax.set_yscale('log')
-
-   ax.legend(loc='best')
-   plt.tight_layout()
-   plt.show()
diff --git a/docs/dust_extinction/references.rst b/docs/dust_extinction/references.rst
index 9a03011..0eb0681 100644
--- a/docs/dust_extinction/references.rst
+++ b/docs/dust_extinction/references.rst
@@ -58,6 +58,9 @@ RL85: `Rieke & Lebofsky 1985, ApJ,288, 618
 VCG04: `Valencic, Clayton, & Gordon 2014, 616, 912
 <https://ui.adsabs.harvard.edu/abs/2004ApJ...616..912V>`_
 
+WG01: `Weingartner & Draine 2001, ApJ, 548, 296
+<https://ui.adsabs.harvard.edu/abs/2001ApJ...548..296W/abstract>`_
+
 ZDA04: `Zubko, Dwek, & Arendt 2004, ApJS, 152, 211
 <https://ui.adsabs.harvard.edu/abs/2004ApJS..152..211Z/abstract>`_
 
diff --git a/dust_extinction/data/kext_albedo_WD_LMC2_10.dat b/dust_extinction/data/kext_albedo_WD_LMC2_10.dat
new file mode 100644
index 0000000..76f768f
--- /dev/null
+++ b/dust_extinction/data/kext_albedo_WD_LMC2_10.dat
@@ -0,0 +1,2444 @@
+Extinction, scattering, and absorption properties computed for the
+carbonaceous - silicate dust model of Weingartner & Draine (2001) and
+Li & Draine (2001).
+
+Model consists of mixture of carbonaceous grains, and amorphous
+silicate grains.  Carbonaceous grains are PAH-like when small, and
+graphite-like when large (see Li & Draine 2001).  Size distributions
+from Weingartner & Draine (2001).  PAH optical properties are from Li
+& Draine (2001).  Graphite and silicate optical properties from Draine
+& Lee (1984), Laor & Draine (1993), Weingartner & Draine (2001), and
+Li & Draine (2001).
+
+Grain size distribution: Weingartner & Draine (2001) model for
+"LMC 2" dust with C/H = b_C = 10.e-6 in two log-normal size
+distributions.
+
+The PAH/graphitic grains in the log-normal size distributions are
+assumed to be 50% neutral and 50% ionized.  The PAH/graphitic grains
+in the size distribution given by eq. (5,6) of Weingartner & Draine
+(2001) are assumed to be 100% ionized.
+
+Calculated by B.T. Draine, Princeton University, 2001.07.05
+
+References:
+Draine, B.T., & Lee, H.-M. 1984, "Optical Properties of Interstellar
+    Graphite and Silicate Grains", Astrophys. J., 285, 89-108
+Laor, A., & Draine, B.T. 1993, "Spectroscopic Constraints on the Properties
+    of Dust in Active Galactic Nuclei", Astrophys. J., 402, 441-468
+Li, A., & Draine, B.T. 2001, "Infrared Emission from Interstellar Dust. II.
+    The Diffuse Interstellar Medium", Astrophys. J., 554, 778-802
+Weingartner, J.C., & Draine, B.T. 2001, "Dust Grain-Size Distributions and 
+    Extinction in the Milky Way, LMC, and SMC", Astrophys. J., 548, 296-309
+
+Tabulated quantities:
+lambda  = wavelength in vacuo (micron) [2401 values from 1.e-2 to 1.e4 um]
+albedo  = (scattering cross section)/(extinction cross section)
+g       = <cos(theta)> for scattered light
+C_ext/H = extinction cross section per H nucleon (cm^2/H)
+K_abs   = absorption cross section per mass of dust (cm^2/gram)
+
+ lambda   albedo    g     C_ext/H    K_abs
+(micron)                  (cm^2/H)  (cm^2/g)
+--------- ------  ------ --------- ---------
+1.000E-02 0.3633  0.9884 2.374E-22 2.665E+04
+1.006E-02 0.3616  0.9883 2.378E-22 2.678E+04
+1.012E-02 0.3598  0.9882 2.382E-22 2.690E+04
+1.017E-02 0.3581  0.9881 2.386E-22 2.702E+04
+1.023E-02 0.3563  0.9879 2.391E-22 2.714E+04
+1.029E-02 0.3545  0.9878 2.395E-22 2.726E+04
+1.035E-02 0.3524  0.9877 2.397E-22 2.738E+04
+1.041E-02 0.3495  0.9877 2.397E-22 2.750E+04
+1.047E-02 0.3464  0.9876 2.397E-22 2.763E+04
+1.053E-02 0.3408  0.9876 2.388E-22 2.776E+04
+1.059E-02 0.3295  0.9879 2.361E-22 2.792E+04
+1.065E-02 0.3281  0.9877 2.367E-22 2.804E+04
+1.072E-02 0.3511  0.9895 2.128E-22 2.435E+04
+1.078E-02 0.3498  0.9894 2.134E-22 2.447E+04
+1.084E-02 0.3621  0.9888 2.182E-22 2.455E+04
+1.090E-02 0.3689  0.9884 2.214E-22 2.464E+04
+1.096E-02 0.3704  0.9882 2.229E-22 2.475E+04
+1.103E-02 0.3718  0.9879 2.244E-22 2.486E+04
+1.109E-02 0.3729  0.9877 2.258E-22 2.497E+04
+1.116E-02 0.3738  0.9875 2.271E-22 2.508E+04
+1.122E-02 0.3746  0.9872 2.284E-22 2.519E+04
+1.128E-02 0.3752  0.9870 2.296E-22 2.531E+04
+1.135E-02 0.3756  0.9868 2.308E-22 2.542E+04
+1.142E-02 0.3759  0.9865 2.319E-22 2.553E+04
+1.148E-02 0.3760  0.9863 2.330E-22 2.564E+04
+1.155E-02 0.3760  0.9861 2.340E-22 2.575E+04
+1.161E-02 0.3759  0.9859 2.350E-22 2.587E+04
+1.168E-02 0.3757  0.9857 2.359E-22 2.598E+04
+1.175E-02 0.3753  0.9855 2.368E-22 2.609E+04
+1.182E-02 0.3748  0.9853 2.377E-22 2.621E+04
+1.189E-02 0.3743  0.9851 2.385E-22 2.632E+04
+1.195E-02 0.3736  0.9849 2.393E-22 2.643E+04
+1.202E-02 0.3728  0.9847 2.400E-22 2.655E+04
+1.209E-02 0.3720  0.9845 2.407E-22 2.666E+04
+1.216E-02 0.3711  0.9843 2.414E-22 2.677E+04
+1.223E-02 0.3701  0.9841 2.420E-22 2.689E+04
+1.230E-02 0.3690  0.9839 2.426E-22 2.700E+04
+1.237E-02 0.3679  0.9837 2.432E-22 2.711E+04
+1.245E-02 0.3667  0.9835 2.438E-22 2.723E+04
+1.252E-02 0.3654  0.9834 2.443E-22 2.734E+04
+1.259E-02 0.3640  0.9832 2.448E-22 2.746E+04
+1.266E-02 0.3626  0.9830 2.453E-22 2.757E+04
+1.274E-02 0.3611  0.9828 2.457E-22 2.769E+04
+1.281E-02 0.3541  0.9830 2.442E-22 2.782E+04
+1.288E-02 0.3641  0.9828 2.433E-22 2.728E+04
+1.296E-02 0.3643  0.9826 2.443E-22 2.739E+04
+1.303E-02 0.3646  0.9823 2.454E-22 2.749E+04
+1.311E-02 0.3642  0.9821 2.462E-22 2.760E+04
+1.318E-02 0.3631  0.9819 2.467E-22 2.771E+04
+1.326E-02 0.3616  0.9817 2.472E-22 2.783E+04
+1.334E-02 0.3598  0.9815 2.475E-22 2.794E+04
+1.341E-02 0.3595  0.9813 2.483E-22 2.804E+04
+1.349E-02 0.3653  0.9815 2.448E-22 2.740E+04
+1.357E-02 0.3660  0.9812 2.460E-22 2.751E+04
+1.365E-02 0.3665  0.9809 2.471E-22 2.761E+04
+1.372E-02 0.3670  0.9806 2.482E-22 2.771E+04
+1.380E-02 0.3671  0.9803 2.492E-22 2.782E+04
+1.388E-02 0.3670  0.9800 2.501E-22 2.792E+04
+1.396E-02 0.3668  0.9797 2.510E-22 2.803E+04
+1.404E-02 0.3665  0.9794 2.518E-22 2.813E+04
+1.413E-02 0.3663  0.9792 2.526E-22 2.824E+04
+1.421E-02 0.3660  0.9789 2.535E-22 2.834E+04
+1.429E-02 0.3656  0.9786 2.543E-22 2.845E+04
+1.437E-02 0.3653  0.9783 2.551E-22 2.856E+04
+1.445E-02 0.3649  0.9780 2.559E-22 2.866E+04
+1.454E-02 0.3645  0.9778 2.567E-22 2.877E+04
+1.462E-02 0.3641  0.9775 2.575E-22 2.888E+04
+1.471E-02 0.3637  0.9772 2.582E-22 2.898E+04
+1.479E-02 0.3632  0.9769 2.590E-22 2.909E+04
+1.488E-02 0.3628  0.9766 2.598E-22 2.919E+04
+1.496E-02 0.3623  0.9763 2.605E-22 2.930E+04
+1.505E-02 0.3619  0.9761 2.613E-22 2.940E+04
+1.514E-02 0.3614  0.9758 2.620E-22 2.951E+04
+1.522E-02 0.3609  0.9755 2.628E-22 2.962E+04
+1.531E-02 0.3604  0.9752 2.635E-22 2.972E+04
+1.540E-02 0.3599  0.9749 2.642E-22 2.983E+04
+1.549E-02 0.3594  0.9746 2.649E-22 2.993E+04
+1.558E-02 0.3589  0.9743 2.657E-22 3.004E+04
+1.567E-02 0.3584  0.9740 2.664E-22 3.014E+04
+1.576E-02 0.3579  0.9737 2.671E-22 3.025E+04
+1.585E-02 0.3574  0.9734 2.678E-22 3.036E+04
+1.594E-02 0.3569  0.9731 2.686E-22 3.046E+04
+1.603E-02 0.3564  0.9727 2.693E-22 3.057E+04
+1.613E-02 0.3558  0.9724 2.700E-22 3.068E+04
+1.622E-02 0.3553  0.9721 2.708E-22 3.079E+04
+1.631E-02 0.3547  0.9718 2.715E-22 3.089E+04
+1.641E-02 0.3542  0.9715 2.722E-22 3.100E+04
+1.650E-02 0.3536  0.9712 2.729E-22 3.111E+04
+1.660E-02 0.3531  0.9708 2.737E-22 3.122E+04
+1.669E-02 0.3526  0.9705 2.744E-22 3.133E+04
+1.679E-02 0.3521  0.9701 2.752E-22 3.144E+04
+1.688E-02 0.3515  0.9698 2.759E-22 3.156E+04
+1.698E-02 0.3509  0.9695 2.766E-22 3.167E+04
+1.708E-02 0.3503  0.9691 2.774E-22 3.178E+04
+1.718E-02 0.3496  0.9688 2.781E-22 3.190E+04
+1.728E-02 0.3490  0.9685 2.789E-22 3.202E+04
+1.738E-02 0.3483  0.9681 2.796E-22 3.213E+04
+1.748E-02 0.3476  0.9678 2.803E-22 3.225E+04
+1.758E-02 0.3469  0.9674 2.810E-22 3.237E+04
+1.768E-02 0.3462  0.9671 2.817E-22 3.249E+04
+1.778E-02 0.3453  0.9667 2.824E-22 3.261E+04
+1.789E-02 0.3443  0.9664 2.831E-22 3.274E+04
+1.799E-02 0.3433  0.9661 2.838E-22 3.286E+04
+1.809E-02 0.3423  0.9658 2.844E-22 3.299E+04
+1.820E-02 0.3412  0.9654 2.851E-22 3.312E+04
+1.830E-02 0.3401  0.9651 2.857E-22 3.325E+04
+1.841E-02 0.3390  0.9648 2.864E-22 3.338E+04
+1.851E-02 0.3379  0.9645 2.870E-22 3.352E+04
+1.862E-02 0.3367  0.9642 2.877E-22 3.365E+04
+1.873E-02 0.3355  0.9638 2.883E-22 3.378E+04
+1.884E-02 0.3335  0.9636 2.886E-22 3.393E+04
+1.895E-02 0.3304  0.9635 2.886E-22 3.409E+04
+1.905E-02 0.3372  0.9648 2.796E-22 3.268E+04
+1.916E-02 0.3378  0.9643 2.807E-22 3.278E+04
+1.928E-02 0.3385  0.9638 2.818E-22 3.288E+04
+1.939E-02 0.3391  0.9632 2.829E-22 3.298E+04
+1.950E-02 0.3396  0.9627 2.840E-22 3.308E+04
+1.961E-02 0.3400  0.9622 2.851E-22 3.319E+04
+1.972E-02 0.3403  0.9616 2.862E-22 3.330E+04
+1.984E-02 0.3406  0.9611 2.872E-22 3.340E+04
+1.995E-02 0.3408  0.9606 2.883E-22 3.352E+04
+2.007E-02 0.3409  0.9601 2.893E-22 3.363E+04
+2.018E-02 0.3410  0.9596 2.903E-22 3.374E+04
+2.030E-02 0.3410  0.9590 2.913E-22 3.386E+04
+2.042E-02 0.3410  0.9585 2.923E-22 3.397E+04
+2.054E-02 0.3408  0.9580 2.932E-22 3.409E+04
+2.065E-02 0.3407  0.9575 2.942E-22 3.421E+04
+2.077E-02 0.3404  0.9570 2.951E-22 3.433E+04
+2.089E-02 0.3402  0.9565 2.961E-22 3.445E+04
+2.101E-02 0.3398  0.9560 2.970E-22 3.458E+04
+2.113E-02 0.3395  0.9555 2.979E-22 3.470E+04
+2.126E-02 0.3391  0.9550 2.988E-22 3.483E+04
+2.138E-02 0.3386  0.9545 2.996E-22 3.495E+04
+2.150E-02 0.3381  0.9540 3.005E-22 3.508E+04
+2.163E-02 0.3377  0.9535 3.014E-22 3.521E+04
+2.175E-02 0.3372  0.9530 3.023E-22 3.533E+04
+2.188E-02 0.3367  0.9525 3.032E-22 3.546E+04
+2.200E-02 0.3363  0.9520 3.040E-22 3.559E+04
+2.213E-02 0.3358  0.9515 3.049E-22 3.572E+04
+2.226E-02 0.3353  0.9509 3.058E-22 3.585E+04
+2.239E-02 0.3347  0.9504 3.067E-22 3.598E+04
+2.252E-02 0.3341  0.9499 3.075E-22 3.612E+04
+2.265E-02 0.3332  0.9495 3.083E-22 3.626E+04
+2.278E-02 0.3321  0.9490 3.091E-22 3.641E+04
+2.291E-02 0.3311  0.9486 3.099E-22 3.656E+04
+2.304E-02 0.3338  0.9487 3.073E-22 3.611E+04
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+7.807E+03 0.0000  0.0000 7.253E-29 1.279E-02
+7.852E+03 0.0000  0.0000 7.185E-29 1.267E-02
+7.898E+03 0.0000  0.0000 7.117E-29 1.255E-02
+7.943E+03 0.0000  0.0000 7.051E-29 1.243E-02
+7.989E+03 0.0000  0.0000 6.984E-29 1.232E-02
+8.035E+03 0.0000  0.0000 6.919E-29 1.220E-02
+8.082E+03 0.0000  0.0000 6.854E-29 1.209E-02
+8.128E+03 0.0000  0.0000 6.789E-29 1.197E-02
+8.175E+03 0.0000  0.0000 6.725E-29 1.186E-02
+8.222E+03 0.0000  0.0000 6.662E-29 1.175E-02
+8.270E+03 0.0000  0.0000 6.600E-29 1.164E-02
+8.318E+03 0.0000  0.0000 6.538E-29 1.153E-02
+8.366E+03 0.0000  0.0000 6.476E-29 1.142E-02
+8.414E+03 0.0000  0.0000 6.416E-29 1.131E-02
+8.463E+03 0.0000  0.0000 6.355E-29 1.121E-02
+8.511E+03 0.0000  0.0000 6.296E-29 1.110E-02
+8.561E+03 0.0000  0.0000 6.237E-29 1.100E-02
+8.610E+03 0.0000  0.0000 6.178E-29 1.090E-02
+8.660E+03 0.0000  0.0000 6.120E-29 1.079E-02
+8.710E+03 0.0000  0.0000 6.063E-29 1.069E-02
+8.760E+03 0.0000  0.0000 6.006E-29 1.059E-02
+8.810E+03 0.0000  0.0000 5.950E-29 1.049E-02
+8.861E+03 0.0000  0.0000 5.894E-29 1.040E-02
+8.913E+03 0.0000  0.0000 5.839E-29 1.030E-02
+8.964E+03 0.0000  0.0000 5.784E-29 1.020E-02
+9.016E+03 0.0000  0.0000 5.730E-29 1.011E-02
+9.068E+03 0.0000  0.0000 5.676E-29 1.001E-02
+9.120E+03 0.0000  0.0000 5.621E-29 9.914E-03
+9.173E+03 0.0000  0.0000 5.568E-29 9.820E-03
+9.226E+03 0.0000  0.0000 5.515E-29 9.726E-03
+9.279E+03 0.0000  0.0000 5.462E-29 9.633E-03
+9.333E+03 0.0000  0.0000 5.410E-29 9.541E-03
+9.386E+03 0.0000  0.0000 5.358E-29 9.450E-03
+9.441E+03 0.0000  0.0000 5.307E-29 9.360E-03
+9.495E+03 0.0000  0.0000 5.256E-29 9.270E-03
+9.550E+03 0.0000  0.0000 5.206E-29 9.182E-03
+9.605E+03 0.0000  0.0000 5.156E-29 9.094E-03
+9.661E+03 0.0000  0.0000 5.107E-29 9.007E-03
+9.716E+03 0.0000  0.0000 5.058E-29 8.920E-03
+9.772E+03 0.0000  0.0000 5.009E-29 8.835E-03
+9.829E+03 0.0000  0.0000 4.961E-29 8.750E-03
+9.886E+03 0.0000  0.0000 4.914E-29 8.666E-03
+9.943E+03 0.0000  0.0000 4.867E-29 8.583E-03
+1.000E+04 0.0000  0.0000 4.820E-29 8.500E-03
diff --git a/dust_extinction/data/kext_albedo_WD_LMCavg_20.dat b/dust_extinction/data/kext_albedo_WD_LMCavg_20.dat
new file mode 100644
index 0000000..38074a8
--- /dev/null
+++ b/dust_extinction/data/kext_albedo_WD_LMCavg_20.dat
@@ -0,0 +1,2444 @@
+Extinction, scattering, and absorption properties computed for the
+carbonaceous - silicate dust model of Weingartner & Draine (2001) and
+Li & Draine (2001).
+
+Model consists of mixture of carbonaceous grains, and amorphous
+silicate grains.  Carbonaceous grains are PAH-like when small, and
+graphite-like when large (see Li & Draine 2001).  Size distributions
+from Weingartner & Draine (2001).  PAH optical properties are from Li
+& Draine (2001).  Graphite and silicate optical properties from Draine
+& Lee (1984), Laor & Draine (1993), Weingartner & Draine (2001), and
+Li & Draine (2001).
+
+Grain size distribution: Weingartner & Draine (2001) model for
+"average LMC" dust with C/H = b_C = 20.e-6 in two log-normal size
+distributions.
+
+The PAH/graphitic grains in the log-normal size distributions are
+assumed to be 50% neutral and 50% ionized.  The PAH/graphitic grains
+in the size distribution given by eq. (5,6) of Weingartner & Draine
+(2001) are assumed to be 100% ionized.
+
+Calculated by B.T. Draine, Princeton University, 2001.07.05
+
+References:
+Draine, B.T., & Lee, H.-M. 1984, "Optical Properties of Interstellar
+    Graphite and Silicate Grains", Astrophys. J., 285, 89-108
+Laor, A., & Draine, B.T. 1993, "Spectroscopic Constraints on the Properties
+    of Dust in Active Galactic Nuclei", Astrophys. J., 402, 441-468
+Li, A., & Draine, B.T. 2001, "Infrared Emission from Interstellar Dust. II.
+    The Diffuse Interstellar Medium", Astrophys. J., 554, 778-802
+Weingartner, J.C., & Draine, B.T. 2001, "Dust Grain-Size Distributions and 
+    Extinction in the Milky Way, LMC, and SMC", Astrophys. J., 548, 296-309
+
+Tabulated quantities:
+lambda  = wavelength in vacuo (micron) [2401 values from 1.e-2 to 1.e4 um]
+albedo  = (scattering cross section)/(extinction cross section)
+g       = <cos(theta)> for scattered light
+C_ext/H = extinction cross section per H nucleon (cm^2/H)
+K_abs   = absorption cross section per mass of dust (cm^2/gram)
+
+ lambda   albedo    g     C_ext/H    K_abs
+(micron)                  (cm^2/H)  (cm^2/g)
+--------- ------  ------ --------- ---------
+1.000E-02 0.3401  0.9866 2.184E-22 2.639E+04
+1.006E-02 0.3383  0.9864 2.189E-22 2.652E+04
+1.012E-02 0.3366  0.9863 2.194E-22 2.665E+04
+1.017E-02 0.3348  0.9862 2.199E-22 2.678E+04
+1.023E-02 0.3330  0.9860 2.204E-22 2.692E+04
+1.029E-02 0.3312  0.9859 2.209E-22 2.705E+04
+1.035E-02 0.3291  0.9858 2.213E-22 2.718E+04
+1.041E-02 0.3262  0.9857 2.214E-22 2.732E+04
+1.047E-02 0.3232  0.9856 2.215E-22 2.745E+04
+1.053E-02 0.3180  0.9856 2.210E-22 2.760E+04
+1.059E-02 0.3076  0.9859 2.190E-22 2.776E+04
+1.065E-02 0.3062  0.9857 2.196E-22 2.789E+04
+1.072E-02 0.3300  0.9877 1.968E-22 2.414E+04
+1.078E-02 0.3286  0.9875 1.974E-22 2.427E+04
+1.084E-02 0.3395  0.9869 2.015E-22 2.437E+04
+1.090E-02 0.3454  0.9865 2.042E-22 2.448E+04
+1.096E-02 0.3466  0.9862 2.056E-22 2.460E+04
+1.103E-02 0.3476  0.9860 2.070E-22 2.472E+04
+1.109E-02 0.3484  0.9857 2.083E-22 2.485E+04
+1.116E-02 0.3491  0.9854 2.095E-22 2.497E+04
+1.122E-02 0.3495  0.9852 2.107E-22 2.510E+04
+1.128E-02 0.3498  0.9849 2.119E-22 2.522E+04
+1.135E-02 0.3500  0.9846 2.130E-22 2.535E+04
+1.142E-02 0.3501  0.9844 2.141E-22 2.547E+04
+1.148E-02 0.3500  0.9841 2.151E-22 2.560E+04
+1.155E-02 0.3498  0.9839 2.161E-22 2.573E+04
+1.161E-02 0.3495  0.9836 2.171E-22 2.586E+04
+1.168E-02 0.3490  0.9834 2.180E-22 2.598E+04
+1.175E-02 0.3485  0.9831 2.189E-22 2.611E+04
+1.182E-02 0.3479  0.9829 2.198E-22 2.624E+04
+1.189E-02 0.3472  0.9827 2.206E-22 2.637E+04
+1.195E-02 0.3464  0.9825 2.214E-22 2.650E+04
+1.202E-02 0.3455  0.9822 2.222E-22 2.663E+04
+1.209E-02 0.3446  0.9820 2.230E-22 2.676E+04
+1.216E-02 0.3435  0.9818 2.237E-22 2.689E+04
+1.223E-02 0.3425  0.9816 2.244E-22 2.701E+04
+1.230E-02 0.3413  0.9814 2.251E-22 2.714E+04
+1.237E-02 0.3401  0.9811 2.257E-22 2.727E+04
+1.245E-02 0.3388  0.9809 2.263E-22 2.740E+04
+1.252E-02 0.3375  0.9807 2.270E-22 2.753E+04
+1.259E-02 0.3361  0.9805 2.276E-22 2.766E+04
+1.266E-02 0.3346  0.9803 2.282E-22 2.780E+04
+1.274E-02 0.3331  0.9801 2.287E-22 2.793E+04
+1.281E-02 0.3266  0.9803 2.277E-22 2.808E+04
+1.288E-02 0.3358  0.9801 2.265E-22 2.754E+04
+1.296E-02 0.3358  0.9798 2.275E-22 2.766E+04
+1.303E-02 0.3359  0.9795 2.286E-22 2.779E+04
+1.311E-02 0.3353  0.9792 2.294E-22 2.792E+04
+1.318E-02 0.3342  0.9790 2.301E-22 2.805E+04
+1.326E-02 0.3327  0.9788 2.306E-22 2.818E+04
+1.334E-02 0.3309  0.9786 2.311E-22 2.831E+04
+1.341E-02 0.3304  0.9783 2.319E-22 2.843E+04
+1.349E-02 0.3359  0.9786 2.286E-22 2.779E+04
+1.357E-02 0.3364  0.9782 2.297E-22 2.792E+04
+1.365E-02 0.3367  0.9779 2.309E-22 2.804E+04
+1.372E-02 0.3368  0.9775 2.320E-22 2.816E+04
+1.380E-02 0.3368  0.9772 2.330E-22 2.829E+04
+1.388E-02 0.3365  0.9769 2.339E-22 2.841E+04
+1.396E-02 0.3361  0.9766 2.348E-22 2.854E+04
+1.404E-02 0.3357  0.9762 2.357E-22 2.867E+04
+1.413E-02 0.3352  0.9759 2.366E-22 2.879E+04
+1.421E-02 0.3348  0.9756 2.375E-22 2.892E+04
+1.429E-02 0.3343  0.9753 2.383E-22 2.905E+04
+1.437E-02 0.3338  0.9750 2.392E-22 2.918E+04
+1.445E-02 0.3333  0.9747 2.401E-22 2.931E+04
+1.454E-02 0.3327  0.9743 2.409E-22 2.944E+04
+1.462E-02 0.3321  0.9740 2.418E-22 2.957E+04
+1.471E-02 0.3316  0.9737 2.426E-22 2.970E+04
+1.479E-02 0.3310  0.9734 2.435E-22 2.982E+04
+1.488E-02 0.3304  0.9730 2.443E-22 2.995E+04
+1.496E-02 0.3298  0.9727 2.452E-22 3.008E+04
+1.505E-02 0.3292  0.9724 2.460E-22 3.022E+04
+1.514E-02 0.3285  0.9721 2.468E-22 3.035E+04
+1.522E-02 0.3279  0.9717 2.477E-22 3.048E+04
+1.531E-02 0.3272  0.9714 2.485E-22 3.061E+04
+1.540E-02 0.3266  0.9711 2.493E-22 3.074E+04
+1.549E-02 0.3259  0.9707 2.502E-22 3.087E+04
+1.558E-02 0.3253  0.9704 2.510E-22 3.100E+04
+1.567E-02 0.3247  0.9700 2.518E-22 3.113E+04
+1.576E-02 0.3240  0.9697 2.526E-22 3.127E+04
+1.585E-02 0.3234  0.9693 2.535E-22 3.140E+04
+1.594E-02 0.3227  0.9690 2.543E-22 3.153E+04
+1.603E-02 0.3221  0.9686 2.551E-22 3.167E+04
+1.613E-02 0.3214  0.9683 2.560E-22 3.181E+04
+1.622E-02 0.3207  0.9679 2.568E-22 3.194E+04
+1.631E-02 0.3200  0.9675 2.577E-22 3.208E+04
+1.641E-02 0.3193  0.9672 2.585E-22 3.222E+04
+1.650E-02 0.3186  0.9668 2.593E-22 3.236E+04
+1.660E-02 0.3180  0.9664 2.602E-22 3.249E+04
+1.669E-02 0.3173  0.9661 2.611E-22 3.263E+04
+1.679E-02 0.3166  0.9657 2.619E-22 3.277E+04
+1.688E-02 0.3159  0.9653 2.628E-22 3.292E+04
+1.698E-02 0.3152  0.9649 2.637E-22 3.306E+04
+1.708E-02 0.3144  0.9645 2.646E-22 3.321E+04
+1.718E-02 0.3137  0.9641 2.654E-22 3.336E+04
+1.728E-02 0.3129  0.9637 2.663E-22 3.350E+04
+1.738E-02 0.3121  0.9633 2.672E-22 3.365E+04
+1.748E-02 0.3112  0.9630 2.680E-22 3.380E+04
+1.758E-02 0.3104  0.9626 2.689E-22 3.395E+04
+1.768E-02 0.3095  0.9622 2.698E-22 3.411E+04
+1.778E-02 0.3086  0.9618 2.706E-22 3.426E+04
+1.789E-02 0.3075  0.9614 2.715E-22 3.442E+04
+1.799E-02 0.3064  0.9610 2.723E-22 3.458E+04
+1.809E-02 0.3053  0.9607 2.732E-22 3.475E+04
+1.820E-02 0.3042  0.9603 2.740E-22 3.491E+04
+1.830E-02 0.3030  0.9599 2.748E-22 3.508E+04
+1.841E-02 0.3018  0.9595 2.757E-22 3.524E+04
+1.851E-02 0.3006  0.9592 2.765E-22 3.541E+04
+1.862E-02 0.2994  0.9588 2.773E-22 3.558E+04
+1.873E-02 0.2981  0.9584 2.782E-22 3.575E+04
+1.884E-02 0.2961  0.9581 2.788E-22 3.593E+04
+1.895E-02 0.2932  0.9580 2.791E-22 3.612E+04
+1.905E-02 0.2995  0.9593 2.703E-22 3.467E+04
+1.916E-02 0.2998  0.9588 2.715E-22 3.481E+04
+1.928E-02 0.3002  0.9582 2.727E-22 3.494E+04
+1.939E-02 0.3004  0.9576 2.739E-22 3.509E+04
+1.950E-02 0.3007  0.9570 2.751E-22 3.523E+04
+1.961E-02 0.3008  0.9564 2.763E-22 3.538E+04
+1.972E-02 0.3009  0.9558 2.775E-22 3.552E+04
+1.984E-02 0.3009  0.9553 2.787E-22 3.568E+04
+1.995E-02 0.3009  0.9547 2.799E-22 3.583E+04
+2.007E-02 0.3007  0.9541 2.810E-22 3.598E+04
+2.018E-02 0.3006  0.9535 2.822E-22 3.614E+04
+2.030E-02 0.3004  0.9530 2.833E-22 3.630E+04
+2.042E-02 0.3001  0.9524 2.845E-22 3.646E+04
+2.054E-02 0.2998  0.9518 2.856E-22 3.662E+04
+2.065E-02 0.2994  0.9513 2.867E-22 3.678E+04
+2.077E-02 0.2990  0.9507 2.878E-22 3.694E+04
+2.089E-02 0.2985  0.9502 2.889E-22 3.711E+04
+2.101E-02 0.2980  0.9496 2.900E-22 3.728E+04
+2.113E-02 0.2974  0.9490 2.911E-22 3.745E+04
+2.126E-02 0.2968  0.9485 2.922E-22 3.762E+04
+2.138E-02 0.2962  0.9479 2.933E-22 3.780E+04
+2.150E-02 0.2956  0.9474 2.944E-22 3.797E+04
+2.163E-02 0.2949  0.9468 2.955E-22 3.814E+04
+2.175E-02 0.2943  0.9463 2.966E-22 3.832E+04
+2.188E-02 0.2937  0.9457 2.977E-22 3.850E+04
+2.200E-02 0.2930  0.9451 2.988E-22 3.867E+04
+2.213E-02 0.2924  0.9446 2.999E-22 3.885E+04
+2.226E-02 0.2917  0.9440 3.010E-22 3.903E+04
+2.239E-02 0.2909  0.9434 3.021E-22 3.922E+04
+2.252E-02 0.2902  0.9429 3.032E-22 3.940E+04
+2.265E-02 0.2892  0.9423 3.042E-22 3.960E+04
+2.278E-02 0.2881  0.9418 3.053E-22 3.979E+04
+2.291E-02 0.2869  0.9413 3.063E-22 4.000E+04
+2.304E-02 0.2891  0.9414 3.039E-22 3.956E+04
+2.317E-02 0.2892  0.9406 3.056E-22 3.977E+04
+2.331E-02 0.2891  0.9397 3.073E-22 4.000E+04
+2.344E-02 0.2888  0.9389 3.089E-22 4.022E+04
+2.358E-02 0.2882  0.9382 3.104E-22 4.045E+04
+2.371E-02 0.2876  0.9374 3.119E-22 4.068E+04
+2.385E-02 0.2870  0.9367 3.133E-22 4.090E+04
+2.399E-02 0.2864  0.9360 3.148E-22 4.113E+04
+2.413E-02 0.2857  0.9353 3.162E-22 4.136E+04
+2.427E-02 0.2850  0.9346 3.177E-22 4.159E+04
+2.441E-02 0.2843  0.9338 3.192E-22 4.182E+04
+2.455E-02 0.2836  0.9331 3.206E-22 4.206E+04
+2.469E-02 0.2828  0.9324 3.221E-22 4.229E+04
+2.483E-02 0.2821  0.9317 3.235E-22 4.253E+04
+2.497E-02 0.2813  0.9309 3.250E-22 4.277E+04
+2.512E-02 0.2806  0.9302 3.265E-22 4.301E+04
+2.526E-02 0.2798  0.9295 3.279E-22 4.325E+04
+2.541E-02 0.2790  0.9287 3.294E-22 4.349E+04
+2.556E-02 0.2782  0.9280 3.309E-22 4.373E+04
+2.570E-02 0.2774  0.9273 3.323E-22 4.397E+04
+2.585E-02 0.2766  0.9265 3.338E-22 4.422E+04
+2.600E-02 0.2758  0.9258 3.353E-22 4.446E+04
+2.615E-02 0.2750  0.9251 3.368E-22 4.471E+04
+2.630E-02 0.2741  0.9243 3.383E-22 4.496E+04
+2.645E-02 0.2733  0.9236 3.398E-22 4.521E+04
+2.661E-02 0.2725  0.9228 3.413E-22 4.546E+04
+2.676E-02 0.2717  0.9221 3.427E-22 4.571E+04
+2.692E-02 0.2708  0.9213 3.442E-22 4.596E+04
+2.707E-02 0.2700  0.9206 3.457E-22 4.621E+04
+2.723E-02 0.2692  0.9198 3.472E-22 4.646E+04
+2.738E-02 0.2684  0.9191 3.487E-22 4.671E+04
+2.754E-02 0.2676  0.9183 3.502E-22 4.696E+04
+2.770E-02 0.2667  0.9176 3.517E-22 4.722E+04
+2.786E-02 0.2659  0.9168 3.532E-22 4.747E+04
+2.802E-02 0.2651  0.9161 3.547E-22 4.773E+04
+2.818E-02 0.2643  0.9153 3.562E-22 4.798E+04
+2.835E-02 0.2634  0.9145 3.577E-22 4.824E+04
+2.851E-02 0.2626  0.9137 3.593E-22 4.851E+04
+2.867E-02 0.2618  0.9130 3.608E-22 4.877E+04
+2.884E-02 0.2609  0.9122 3.624E-22 4.904E+04
+2.901E-02 0.2601  0.9114 3.639E-22 4.930E+04
+2.917E-02 0.2593  0.9106 3.655E-22 4.957E+04
+2.934E-02 0.2584  0.9099 3.670E-22 4.984E+04
+2.951E-02 0.2576  0.9091 3.686E-22 5.011E+04
+2.968E-02 0.2567  0.9083 3.702E-22 5.038E+04
+2.985E-02 0.2559  0.9075 3.718E-22 5.065E+04
+3.003E-02 0.2551  0.9067 3.734E-22 5.092E+04
+3.020E-02 0.2542  0.9059 3.750E-22 5.120E+04
+3.037E-02 0.2534  0.9051 3.765E-22 5.147E+04
+3.055E-02 0.2526  0.9043 3.781E-22 5.175E+04
+3.073E-02 0.2517  0.9035 3.797E-22 5.202E+04
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diff --git a/dust_extinction/data/kext_albedo_WD_MW_3.1_60.dat b/dust_extinction/data/kext_albedo_WD_MW_3.1_60.dat
new file mode 100644
index 0000000..673a2a0
--- /dev/null
+++ b/dust_extinction/data/kext_albedo_WD_MW_3.1_60.dat
@@ -0,0 +1,2451 @@
+Extinction, scattering, and absorption properties computed for the
+carbonaceous - silicate dust model of Weingartner & Draine (2001) and
+Li & Draine (2001).
+
+Model consists of mixture of carbonaceous grains, and amorphous
+silicate grains.  Carbonaceous grains are PAH-like when small, and
+graphite-like when large (see Li & Draine 2001).  Size distributions
+from Weingartner & Draine (2001).  PAH optical properties are from Li
+& Draine (2001).  Graphite and silicate optical properties from Draine
+& Lee (1984), Laor & Draine (1993), Weingartner & Draine (2001), and
+Li & Draine (2001).
+
+Grain size distribution: Weingartner & Draine (2001) model for
+R_V=3.1 galactic dust with C/H = b_C = 60.e-6 in two log-normal size
+distributions.
+
+The PAH/graphitic grains in the log-normal size distributions are
+assumed to be 50% neutral and 50% ionized.  The PAH/graphitic grains
+in the size distribution given by eq. (5,6) of Weingartner & Draine
+(2001) are assumed to be 100% ionized.
+
+**************************** NOTE ***********************************
+C_ext/H and K_abs published in Table 6 of Li & Draine (2001) are too
+small by a factor of 1.086 (see erratum, Li & Draine 2001b).
+
+This table is an extended and corrected version of Table 6 from Li & 
+Draine (2001), recalculated by B.T. Draine 2001.07.05
+
+*********************************************************************
+
+References:
+Draine, B.T., & Lee, H.-M. 1984, "Optical Properties of Interstellar
+    Graphite and Silicate Grains", Astrophys. J., 285, 89-108
+Laor, A., & Draine, B.T. 1993, "Spectroscopic Constraints on the Properties
+    of Dust in Active Galactic Nuclei", Astrophys. J., 402, 441-468
+Li, A., & Draine, B.T. 2001, "Infrared Emission from Interstellar Dust. II.
+    The Diffuse Interstellar Medium", Astrophys. J., 554, 778-802
+Weingartner, J.C., & Draine, B.T. 2001, "Dust Grain-Size Distributions and 
+    Extinction in the Milky Way, LMC, and SMC", Astrophys. J., 548, 296-309
+
+Tabulated quantities:
+lambda  = wavelength in vacuo (micron)
+albedo  = (scattering cross section)/(extinction cross section)
+g       = <cos(theta)> for scattered light
+C_ext/H = extinction cross section per H nucleon (cm^2/H)
+K_abs   = absorption cross section per mass of dust (cm^2/gram)
+
+ lambda   albedo    g     C_ext/H    K_abs
+(micron)                  (cm^2/H)  (cm^2/g)
+--------- ------  ------ --------- ---------
+1.000E-02 0.4711  0.9928 7.146E-22 2.085E+04
+1.006E-02 0.4696  0.9928 7.158E-22 2.095E+04
+1.012E-02 0.4680  0.9927 7.170E-22 2.104E+04
+1.017E-02 0.4665  0.9926 7.181E-22 2.114E+04
+1.023E-02 0.4649  0.9925 7.193E-22 2.123E+04
+1.029E-02 0.4634  0.9924 7.204E-22 2.133E+04
+1.035E-02 0.4616  0.9923 7.212E-22 2.142E+04
+1.041E-02 0.4592  0.9923 7.213E-22 2.152E+04
+1.047E-02 0.4567  0.9922 7.214E-22 2.162E+04
+1.053E-02 0.4524  0.9922 7.193E-22 2.173E+04
+1.059E-02 0.4441  0.9923 7.128E-22 2.186E+04
+1.065E-02 0.4428  0.9922 7.142E-22 2.196E+04
+1.072E-02 0.4630  0.9930 6.722E-22 1.992E+04
+1.078E-02 0.4616  0.9929 6.738E-22 2.001E+04
+1.084E-02 0.4697  0.9926 6.863E-22 2.008E+04
+1.090E-02 0.4740  0.9923 6.945E-22 2.016E+04
+1.096E-02 0.4746  0.9922 6.985E-22 2.025E+04
+1.103E-02 0.4751  0.9920 7.024E-22 2.034E+04
+1.109E-02 0.4755  0.9918 7.060E-22 2.043E+04
+1.116E-02 0.4757  0.9917 7.095E-22 2.052E+04
+1.122E-02 0.4758  0.9915 7.128E-22 2.061E+04
+1.128E-02 0.4758  0.9914 7.160E-22 2.071E+04
+1.135E-02 0.4757  0.9912 7.191E-22 2.080E+04
+1.142E-02 0.4755  0.9910 7.221E-22 2.090E+04
+1.148E-02 0.4752  0.9909 7.249E-22 2.099E+04
+1.155E-02 0.4748  0.9907 7.276E-22 2.108E+04
+1.161E-02 0.4743  0.9906 7.302E-22 2.118E+04
+1.168E-02 0.4737  0.9904 7.327E-22 2.128E+04
+1.175E-02 0.4730  0.9903 7.351E-22 2.137E+04
+1.182E-02 0.4723  0.9901 7.373E-22 2.147E+04
+1.189E-02 0.4715  0.9900 7.395E-22 2.156E+04
+1.195E-02 0.4706  0.9898 7.416E-22 2.166E+04
+1.202E-02 0.4697  0.9897 7.436E-22 2.176E+04
+1.209E-02 0.4687  0.9895 7.455E-22 2.185E+04
+1.216E-02 0.4677  0.9894 7.473E-22 2.195E+04
+1.223E-02 0.4666  0.9892 7.491E-22 2.204E+04
+1.230E-02 0.4655  0.9891 7.507E-22 2.214E+04
+1.237E-02 0.4643  0.9889 7.523E-22 2.224E+04
+1.245E-02 0.4631  0.9888 7.539E-22 2.233E+04
+1.252E-02 0.4618  0.9886 7.554E-22 2.243E+04
+1.259E-02 0.4604  0.9885 7.569E-22 2.253E+04
+1.266E-02 0.4590  0.9883 7.583E-22 2.263E+04
+1.274E-02 0.4576  0.9882 7.596E-22 2.273E+04
+1.281E-02 0.4523  0.9882 7.563E-22 2.285E+04
+1.288E-02 0.4593  0.9881 7.569E-22 2.258E+04
+1.296E-02 0.4590  0.9879 7.596E-22 2.267E+04
+1.303E-02 0.4588  0.9877 7.625E-22 2.277E+04
+1.311E-02 0.4581  0.9875 7.646E-22 2.286E+04
+1.318E-02 0.4570  0.9873 7.663E-22 2.296E+04
+1.326E-02 0.4555  0.9872 7.676E-22 2.306E+04
+1.334E-02 0.4539  0.9870 7.686E-22 2.316E+04
+1.341E-02 0.4532  0.9868 7.709E-22 2.325E+04
+1.349E-02 0.4573  0.9868 7.661E-22 2.294E+04
+1.357E-02 0.4573  0.9866 7.692E-22 2.303E+04
+1.365E-02 0.4573  0.9864 7.723E-22 2.312E+04
+1.372E-02 0.4571  0.9861 7.752E-22 2.322E+04
+1.380E-02 0.4568  0.9859 7.778E-22 2.331E+04
+1.388E-02 0.4563  0.9857 7.802E-22 2.341E+04
+1.396E-02 0.4557  0.9855 7.826E-22 2.350E+04
+1.404E-02 0.4551  0.9852 7.849E-22 2.360E+04
+1.413E-02 0.4545  0.9850 7.872E-22 2.369E+04
+1.421E-02 0.4538  0.9848 7.895E-22 2.379E+04
+1.429E-02 0.4532  0.9846 7.918E-22 2.389E+04
+1.437E-02 0.4525  0.9843 7.940E-22 2.399E+04
+1.445E-02 0.4518  0.9841 7.963E-22 2.408E+04
+1.454E-02 0.4511  0.9839 7.985E-22 2.418E+04
+1.462E-02 0.4504  0.9836 8.006E-22 2.428E+04
+1.471E-02 0.4496  0.9834 8.028E-22 2.438E+04
+1.479E-02 0.4489  0.9832 8.049E-22 2.447E+04
+1.488E-02 0.4481  0.9829 8.071E-22 2.457E+04
+1.496E-02 0.4474  0.9827 8.092E-22 2.467E+04
+1.505E-02 0.4466  0.9824 8.113E-22 2.477E+04
+1.514E-02 0.4458  0.9822 8.135E-22 2.487E+04
+1.522E-02 0.4450  0.9819 8.156E-22 2.497E+04
+1.531E-02 0.4442  0.9817 8.177E-22 2.507E+04
+1.540E-02 0.4434  0.9814 8.198E-22 2.517E+04
+1.549E-02 0.4426  0.9812 8.219E-22 2.527E+04
+1.558E-02 0.4419  0.9809 8.239E-22 2.537E+04
+1.567E-02 0.4411  0.9807 8.260E-22 2.547E+04
+1.576E-02 0.4403  0.9804 8.281E-22 2.557E+04
+1.585E-02 0.4395  0.9801 8.302E-22 2.567E+04
+1.594E-02 0.4387  0.9799 8.323E-22 2.578E+04
+1.603E-02 0.4379  0.9796 8.344E-22 2.588E+04
+1.613E-02 0.4371  0.9793 8.366E-22 2.598E+04
+1.622E-02 0.4363  0.9790 8.387E-22 2.608E+04
+1.631E-02 0.4354  0.9787 8.408E-22 2.619E+04
+1.641E-02 0.4346  0.9785 8.429E-22 2.629E+04
+1.650E-02 0.4338  0.9782 8.450E-22 2.640E+04
+1.660E-02 0.4330  0.9779 8.471E-22 2.650E+04
+1.669E-02 0.4322  0.9776 8.493E-22 2.661E+04
+1.679E-02 0.4314  0.9773 8.515E-22 2.671E+04
+1.688E-02 0.4305  0.9770 8.536E-22 2.682E+04
+1.698E-02 0.4297  0.9767 8.558E-22 2.693E+04
+1.708E-02 0.4288  0.9764 8.580E-22 2.704E+04
+1.718E-02 0.4279  0.9760 8.601E-22 2.715E+04
+1.728E-02 0.4270  0.9757 8.623E-22 2.726E+04
+1.738E-02 0.4261  0.9754 8.644E-22 2.737E+04
+1.748E-02 0.4251  0.9751 8.665E-22 2.748E+04
+1.758E-02 0.4242  0.9748 8.687E-22 2.760E+04
+1.768E-02 0.4232  0.9745 8.708E-22 2.771E+04
+1.778E-02 0.4222  0.9742 8.728E-22 2.783E+04
+1.789E-02 0.4211  0.9738 8.748E-22 2.794E+04
+1.799E-02 0.4199  0.9735 8.768E-22 2.806E+04
+1.809E-02 0.4188  0.9732 8.788E-22 2.818E+04
+1.820E-02 0.4176  0.9729 8.808E-22 2.830E+04
+1.830E-02 0.4164  0.9726 8.828E-22 2.843E+04
+1.841E-02 0.4151  0.9723 8.848E-22 2.855E+04
+1.851E-02 0.4139  0.9719 8.868E-22 2.868E+04
+1.862E-02 0.4126  0.9716 8.887E-22 2.880E+04
+1.873E-02 0.4113  0.9713 8.907E-22 2.893E+04
+1.884E-02 0.4095  0.9710 8.920E-22 2.906E+04
+1.895E-02 0.4068  0.9708 8.924E-22 2.921E+04
+1.905E-02 0.4113  0.9713 8.784E-22 2.853E+04
+1.916E-02 0.4112  0.9708 8.815E-22 2.863E+04
+1.928E-02 0.4113  0.9704 8.848E-22 2.874E+04
+1.939E-02 0.4112  0.9699 8.880E-22 2.885E+04
+1.950E-02 0.4111  0.9695 8.912E-22 2.896E+04
+1.961E-02 0.4109  0.9690 8.944E-22 2.907E+04
+1.972E-02 0.4107  0.9686 8.975E-22 2.918E+04
+1.984E-02 0.4104  0.9681 9.005E-22 2.929E+04
+1.995E-02 0.4101  0.9676 9.036E-22 2.941E+04
+2.007E-02 0.4097  0.9672 9.065E-22 2.952E+04
+2.018E-02 0.4093  0.9667 9.095E-22 2.964E+04
+2.030E-02 0.4089  0.9663 9.124E-22 2.976E+04
+2.042E-02 0.4084  0.9658 9.153E-22 2.987E+04
+2.054E-02 0.4079  0.9653 9.181E-22 2.999E+04
+2.065E-02 0.4073  0.9649 9.209E-22 3.011E+04
+2.077E-02 0.4067  0.9644 9.238E-22 3.024E+04
+2.089E-02 0.4060  0.9639 9.266E-22 3.036E+04
+2.101E-02 0.4054  0.9635 9.294E-22 3.049E+04
+2.113E-02 0.4046  0.9630 9.321E-22 3.062E+04
+2.126E-02 0.4039  0.9625 9.348E-22 3.075E+04
+2.138E-02 0.4031  0.9621 9.376E-22 3.087E+04
+2.150E-02 0.4023  0.9616 9.402E-22 3.100E+04
+2.163E-02 0.4016  0.9611 9.430E-22 3.113E+04
+2.175E-02 0.4008  0.9607 9.457E-22 3.126E+04
+2.188E-02 0.4000  0.9602 9.485E-22 3.140E+04
+2.200E-02 0.3992  0.9597 9.512E-22 3.153E+04
+2.213E-02 0.3984  0.9592 9.540E-22 3.166E+04
+2.226E-02 0.3976  0.9587 9.568E-22 3.180E+04
+2.239E-02 0.3967  0.9582 9.596E-22 3.194E+04
+2.252E-02 0.3958  0.9577 9.623E-22 3.208E+04
+2.265E-02 0.3948  0.9572 9.649E-22 3.222E+04
+2.278E-02 0.3936  0.9568 9.674E-22 3.237E+04
+2.291E-02 0.3924  0.9563 9.700E-22 3.252E+04
+2.304E-02 0.3937  0.9561 9.673E-22 3.236E+04
+2.317E-02 0.3935  0.9554 9.714E-22 3.250E+04
+2.331E-02 0.3932  0.9548 9.754E-22 3.266E+04
+2.344E-02 0.3927  0.9542 9.793E-22 3.281E+04
+2.358E-02 0.3920  0.9535 9.830E-22 3.297E+04
+2.371E-02 0.3913  0.9529 9.865E-22 3.313E+04
+2.385E-02 0.3905  0.9523 9.900E-22 3.329E+04
+2.399E-02 0.3897  0.9517 9.935E-22 3.345E+04
+2.413E-02 0.3889  0.9511 9.970E-22 3.361E+04
+2.427E-02 0.3881  0.9505 1.000E-21 3.378E+04
+2.441E-02 0.3873  0.9499 1.004E-21 3.394E+04
+2.455E-02 0.3864  0.9493 1.008E-21 3.411E+04
+2.469E-02 0.3856  0.9487 1.011E-21 3.427E+04
+2.483E-02 0.3847  0.9480 1.015E-21 3.444E+04
+2.497E-02 0.3838  0.9474 1.018E-21 3.461E+04
+2.512E-02 0.3829  0.9468 1.022E-21 3.478E+04
+2.526E-02 0.3820  0.9462 1.025E-21 3.495E+04
+2.541E-02 0.3811  0.9455 1.029E-21 3.512E+04
+2.556E-02 0.3802  0.9449 1.032E-21 3.530E+04
+2.570E-02 0.3793  0.9442 1.036E-21 3.547E+04
+2.585E-02 0.3784  0.9436 1.039E-21 3.565E+04
+2.600E-02 0.3775  0.9430 1.043E-21 3.582E+04
+2.615E-02 0.3765  0.9423 1.047E-21 3.600E+04
+2.630E-02 0.3756  0.9417 1.050E-21 3.618E+04
+2.645E-02 0.3747  0.9410 1.054E-21 3.636E+04
+2.661E-02 0.3737  0.9403 1.057E-21 3.654E+04
+2.676E-02 0.3728  0.9397 1.061E-21 3.672E+04
+2.692E-02 0.3718  0.9390 1.065E-21 3.690E+04
+2.707E-02 0.3709  0.9384 1.068E-21 3.708E+04
+2.723E-02 0.3699  0.9377 1.072E-21 3.726E+04
+2.738E-02 0.3690  0.9370 1.076E-21 3.744E+04
+2.754E-02 0.3681  0.9363 1.079E-21 3.763E+04
+2.770E-02 0.3671  0.9357 1.083E-21 3.781E+04
+2.786E-02 0.3662  0.9350 1.087E-21 3.800E+04
+2.802E-02 0.3652  0.9343 1.090E-21 3.819E+04
+2.818E-02 0.3643  0.9336 1.094E-21 3.838E+04
+2.835E-02 0.3633  0.9329 1.098E-21 3.857E+04
+2.851E-02 0.3623  0.9322 1.102E-21 3.876E+04
+2.867E-02 0.3614  0.9315 1.106E-21 3.895E+04
+2.884E-02 0.3604  0.9308 1.109E-21 3.915E+04
+2.901E-02 0.3594  0.9301 1.113E-21 3.934E+04
+2.917E-02 0.3584  0.9294 1.117E-21 3.954E+04
+2.934E-02 0.3575  0.9286 1.121E-21 3.974E+04
+2.951E-02 0.3565  0.9279 1.125E-21 3.994E+04
+2.968E-02 0.3555  0.9272 1.129E-21 4.014E+04
+2.985E-02 0.3545  0.9265 1.133E-21 4.035E+04
+3.003E-02 0.3535  0.9257 1.137E-21 4.055E+04
+3.020E-02 0.3525  0.9250 1.141E-21 4.076E+04
+3.037E-02 0.3515  0.9243 1.145E-21 4.096E+04
+3.055E-02 0.3505  0.9236 1.149E-21 4.117E+04
+3.073E-02 0.3496  0.9228 1.153E-21 4.137E+04
+3.090E-02 0.3486  0.9221 1.157E-21 4.158E+04
+3.108E-02 0.3476  0.9213 1.161E-21 4.179E+04
+3.126E-02 0.3466  0.9206 1.165E-21 4.200E+04
+3.144E-02 0.3457  0.9198 1.169E-21 4.221E+04
+3.162E-02 0.3447  0.9191 1.173E-21 4.242E+04
+3.181E-02 0.3437  0.9183 1.177E-21 4.264E+04
+3.199E-02 0.3427  0.9176 1.182E-21 4.285E+04
+3.217E-02 0.3418  0.9168 1.186E-21 4.306E+04
+3.236E-02 0.3408  0.9161 1.190E-21 4.328E+04
+3.255E-02 0.3398  0.9153 1.194E-21 4.350E+04
+3.273E-02 0.3388  0.9146 1.198E-21 4.371E+04
+3.292E-02 0.3378  0.9138 1.203E-21 4.393E+04
+3.311E-02 0.3368  0.9131 1.207E-21 4.415E+04
+3.330E-02 0.3359  0.9123 1.211E-21 4.437E+04
+3.350E-02 0.3349  0.9116 1.215E-21 4.459E+04
+3.369E-02 0.3339  0.9108 1.219E-21 4.481E+04
+3.388E-02 0.3329  0.9101 1.224E-21 4.504E+04
+3.408E-02 0.3319  0.9093 1.228E-21 4.526E+04
+3.428E-02 0.3309  0.9086 1.232E-21 4.549E+04
+3.447E-02 0.3299  0.9078 1.236E-21 4.571E+04
+3.467E-02 0.3289  0.9070 1.241E-21 4.594E+04
+3.487E-02 0.3279  0.9063 1.245E-21 4.617E+04
+3.508E-02 0.3269  0.9056 1.249E-21 4.640E+04
+3.528E-02 0.3259  0.9049 1.254E-21 4.662E+04
+3.548E-02 0.3247  0.9043 1.258E-21 4.687E+04
+3.569E-02 0.3232  0.9037 1.263E-21 4.716E+04
+3.589E-02 0.3219  0.9032 1.267E-21 4.741E+04
+3.610E-02 0.3208  0.9028 1.271E-21 4.761E+04
+3.631E-02 0.3200  0.9023 1.273E-21 4.777E+04
+3.652E-02 0.3196  0.9019 1.274E-21 4.783E+04
+3.673E-02 0.3202  0.9015 1.271E-21 4.768E+04
+3.694E-02 0.3209  0.9011 1.268E-21 4.752E+04
+3.715E-02 0.3219  0.9006 1.265E-21 4.733E+04
+3.737E-02 0.3230  0.9001 1.261E-21 4.711E+04
+3.758E-02 0.3243  0.8994 1.258E-21 4.689E+04
+3.780E-02 0.3252  0.8986 1.257E-21 4.678E+04
+3.802E-02 0.3260  0.8976 1.256E-21 4.670E+04
+3.824E-02 0.3268  0.8966 1.256E-21 4.665E+04
+3.846E-02 0.3275  0.8955 1.256E-21 4.661E+04
+3.868E-02 0.3282  0.8943 1.257E-21 4.660E+04
+3.890E-02 0.3287  0.8931 1.258E-21 4.661E+04
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+9.333E+03 0.0000  0.0000 1.613E-28 8.898E-03
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+9.441E+03 0.0000  0.0000 1.581E-28 8.725E-03
+9.495E+03 0.0000  0.0000 1.566E-28 8.639E-03
+9.550E+03 0.0000  0.0000 1.551E-28 8.555E-03
+9.605E+03 0.0000  0.0000 1.535E-28 8.471E-03
+9.661E+03 0.0000  0.0000 1.520E-28 8.388E-03
+9.716E+03 0.0000  0.0000 1.505E-28 8.305E-03
+9.772E+03 0.0000  0.0000 1.491E-28 8.224E-03
+9.829E+03 0.0000  0.0000 1.476E-28 8.143E-03
+9.886E+03 0.0000  0.0000 1.461E-28 8.063E-03
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diff --git a/dust_extinction/data/kext_albedo_WD_MW_4.0B_40.dat b/dust_extinction/data/kext_albedo_WD_MW_4.0B_40.dat
new file mode 100644
index 0000000..8d8c7c7
--- /dev/null
+++ b/dust_extinction/data/kext_albedo_WD_MW_4.0B_40.dat
@@ -0,0 +1,2444 @@
+Extinction, scattering, and absorption properties computed for the
+carbonaceous - silicate dust model of Weingartner & Draine (2001) and
+Li & Draine (2001).
+
+Model consists of mixture of carbonaceous grains, and amorphous
+silicate grains.  Carbonaceous grains are PAH-like when small, and
+graphite-like when large (see Li & Draine 2001).  Size distributions
+from Weingartner & Draine (2001).  PAH optical properties are from Li
+& Draine (2001).  Graphite and silicate optical properties from Draine
+& Lee (1984), Laor & Draine (1993), Weingartner & Draine (2001), and
+Li & Draine (2001).
+
+Grain size distribution: Weingartner & Draine (2001) model B for
+R_V=4.0 galactic dust with C/H = b_C = 40.e-6 in two log-normal size
+distributions.
+
+The PAH/graphitic grains in the log-normal size distributions are
+assumed to be 50% neutral and 50% ionized.  The PAH/graphitic grains
+in the size distribution given by eq. (5,6) of Weingartner & Draine
+(2001) are assumed to be 100% ionized.
+
+Calculated by B.T. Draine, Princeton University, 2001.07.05
+
+References:
+Draine, B.T., & Lee, H.-M. 1984, "Optical Properties of Interstellar
+    Graphite and Silicate Grains", Astrophys. J., 285, 89-108
+Laor, A., & Draine, B.T. 1993, "Spectroscopic Constraints on the Properties
+    of Dust in Active Galactic Nuclei", Astrophys. J., 402, 441-468
+Li, A., & Draine, B.T. 2001, "Infrared Emission from Interstellar Dust. II.
+    The Diffuse Interstellar Medium", Astrophys. J., 554, 778-802
+Weingartner, J.C., & Draine, B.T. 2001, "Dust Grain-Size Distributions and 
+    Extinction in the Milky Way, LMC, and SMC", Astrophys. J., 548, 296-309
+
+Tabulated quantities:
+lambda  = wavelength in vacuo (micron) [2401 values from 1.e-2 to 1.e4 um]
+albedo  = (scattering cross section)/(extinction cross section)
+g       = <cos(theta)> for scattered light
+C_ext/H = extinction cross section per H nucleon (cm^2/H)
+K_abs   = absorption cross section per mass of dust (cm^2/gram)
+
+ lambda   albedo    g     C_ext/H    K_abs
+(micron)                  (cm^2/H)  (cm^2/g)
+--------- ------  ------ --------- ---------
+1.000E-02 0.4947  0.9945 5.258E-22 1.477E+04
+1.006E-02 0.4934  0.9944 5.263E-22 1.483E+04
+1.012E-02 0.4922  0.9943 5.269E-22 1.488E+04
+1.017E-02 0.4909  0.9943 5.274E-22 1.493E+04
+1.023E-02 0.4897  0.9942 5.280E-22 1.498E+04
+1.029E-02 0.4884  0.9941 5.285E-22 1.504E+04
+1.035E-02 0.4869  0.9941 5.288E-22 1.509E+04
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+9.550E+03 0.0000 -0.1021 6.710E-28 3.732E-02
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+9.661E+03 0.0000 -0.1016 6.616E-28 3.680E-02
+9.716E+03 0.0000 -0.1014 6.570E-28 3.654E-02
+9.772E+03 0.0000 -0.1011 6.523E-28 3.628E-02
+9.829E+03 0.0000 -0.1009 6.477E-28 3.602E-02
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diff --git a/dust_extinction/data/kext_albedo_WD_MW_5.5B_30.dat b/dust_extinction/data/kext_albedo_WD_MW_5.5B_30.dat
new file mode 100644
index 0000000..55d5ef8
--- /dev/null
+++ b/dust_extinction/data/kext_albedo_WD_MW_5.5B_30.dat
@@ -0,0 +1,2444 @@
+Extinction, scattering, and absorption properties computed for the
+carbonaceous - silicate dust model of Weingartner & Draine (2001) and
+Li & Draine (2001).
+
+Model consists of mixture of carbonaceous grains, and amorphous
+silicate grains.  Carbonaceous grains are PAH-like when small, and
+graphite-like when large (see Li & Draine 2001).  Size distributions
+from Weingartner & Draine (2001).  PAH optical properties are from Li
+& Draine (2001).  Graphite and silicate optical properties from Draine
+& Lee (1984), Laor & Draine (1993), Weingartner & Draine (2001), and
+Li & Draine (2001).
+
+Grain size distribution: Weingartner & Draine (2001) model B for
+R_V=5.5 galactic dust with C/H = b_C = 30.e-6 in two log-normal size
+distributions.
+
+The PAH/graphitic grains in the log-normal size distributions are
+assumed to be 50% neutral and 50% ionized.  The PAH/graphitic grains
+in the size distribution given by eq. (5,6) of Weingartner & Draine
+(2001) are assumed to be 100% ionized.
+
+Calculated by B.T. Draine, Princeton University, 2001.07.05
+
+References:
+Draine, B.T., & Lee, H.-M. 1984, "Optical Properties of Interstellar
+    Graphite and Silicate Grains", Astrophys. J., 285, 89-108
+Laor, A., & Draine, B.T. 1993, "Spectroscopic Constraints on the Properties
+    of Dust in Active Galactic Nuclei", Astrophys. J., 402, 441-468
+Li, A., & Draine, B.T. 2001, "Infrared Emission from Interstellar Dust. II.
+    The Diffuse Interstellar Medium", Astrophys. J., 554, 778-802
+Weingartner, J.C., & Draine, B.T. 2001, "Dust Grain-Size Distributions and 
+    Extinction in the Milky Way, LMC, and SMC", Astrophys. J., 548, 296-309
+
+Tabulated quantities:
+lambda  = wavelength in vacuo (micron) [2401 values from 1.e-2 to 1.e4 um]
+albedo  = (scattering cross section)/(extinction cross section)
+g       = <cos(theta)> for scattered light
+C_ext/H = extinction cross section per H nucleon (cm^2/H)
+K_abs   = absorption cross section per mass of dust (cm^2/gram)
+
+ lambda   albedo    g     C_ext/H    K_abs
+(micron)                  (cm^2/H)  (cm^2/g)
+--------- ------  ------ --------- ---------
+1.000E-02 0.5156  0.9962 4.195E-22 1.130E+04
+1.006E-02 0.5145  0.9962 4.196E-22 1.133E+04
+1.012E-02 0.5135  0.9961 4.197E-22 1.135E+04
+1.017E-02 0.5124  0.9961 4.198E-22 1.138E+04
+1.023E-02 0.5113  0.9960 4.199E-22 1.141E+04
+1.029E-02 0.5102  0.9960 4.199E-22 1.144E+04
+1.035E-02 0.5089  0.9960 4.199E-22 1.147E+04
+1.041E-02 0.5072  0.9959 4.195E-22 1.150E+04
+1.047E-02 0.5054  0.9959 4.191E-22 1.153E+04
+1.053E-02 0.5023  0.9959 4.178E-22 1.156E+04
+1.059E-02 0.4957  0.9959 4.142E-22 1.161E+04
+1.065E-02 0.4948  0.9959 4.144E-22 1.164E+04
+1.072E-02 0.5070  0.9962 4.083E-22 1.119E+04
+1.078E-02 0.5061  0.9961 4.086E-22 1.122E+04
+1.084E-02 0.5127  0.9960 4.143E-22 1.123E+04
+1.090E-02 0.5160  0.9958 4.177E-22 1.124E+04
+1.096E-02 0.5166  0.9957 4.191E-22 1.126E+04
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+5.158E+03 0.0000 -0.2020 2.043E-27 1.136E-01
+5.188E+03 0.0000 -0.2020 2.034E-27 1.131E-01
+5.218E+03 0.0000 -0.2019 2.025E-27 1.126E-01
+5.248E+03 0.0000 -0.2018 2.016E-27 1.121E-01
+5.278E+03 0.0000 -0.2018 2.007E-27 1.116E-01
+5.309E+03 0.0000 -0.2017 1.998E-27 1.111E-01
+5.339E+03 0.0000 -0.2016 1.989E-27 1.106E-01
+5.370E+03 0.0000 -0.2016 1.980E-27 1.101E-01
+5.401E+03 0.0000 -0.2015 1.971E-27 1.096E-01
+5.433E+03 0.0000 -0.2015 1.962E-27 1.091E-01
+5.464E+03 0.0000 -0.2014 1.954E-27 1.086E-01
+5.495E+03 0.0000 -0.2013 1.945E-27 1.081E-01
+5.527E+03 0.0000 -0.2012 1.936E-27 1.077E-01
+5.559E+03 0.0000 -0.2012 1.927E-27 1.072E-01
+5.591E+03 0.0000 -0.2011 1.919E-27 1.067E-01
+5.623E+03 0.0000 -0.2010 1.910E-27 1.062E-01
+5.656E+03 0.0000 -0.2010 1.902E-27 1.057E-01
+5.689E+03 0.0000 -0.2009 1.893E-27 1.053E-01
+5.721E+03 0.0000 -0.2008 1.884E-27 1.048E-01
+5.754E+03 0.0000 -0.2008 1.876E-27 1.043E-01
+5.788E+03 0.0000 -0.2007 1.867E-27 1.038E-01
+5.821E+03 0.0000 -0.2006 1.859E-27 1.034E-01
+5.855E+03 0.0000 -0.2005 1.851E-27 1.029E-01
+5.888E+03 0.0000 -0.2005 1.842E-27 1.024E-01
+5.922E+03 0.0000 -0.2004 1.834E-27 1.020E-01
+5.957E+03 0.0000 -0.2003 1.825E-27 1.015E-01
+5.991E+03 0.0000 -0.2002 1.817E-27 1.010E-01
+6.026E+03 0.0000 -0.2002 1.809E-27 1.006E-01
+6.060E+03 0.0000 -0.2001 1.801E-27 1.001E-01
+6.095E+03 0.0000 -0.2000 1.792E-27 9.967E-02
+6.131E+03 0.0000 -0.1999 1.784E-27 9.922E-02
+6.166E+03 0.0000 -0.1999 1.776E-27 9.876E-02
+6.202E+03 0.0000 -0.1998 1.768E-27 9.831E-02
+6.237E+03 0.0000 -0.1997 1.760E-27 9.786E-02
+6.273E+03 0.0000 -0.1996 1.752E-27 9.741E-02
+6.310E+03 0.0000 -0.1995 1.744E-27 9.697E-02
+6.346E+03 0.0000 -0.1994 1.736E-27 9.652E-02
+6.383E+03 0.0000 -0.1994 1.728E-27 9.608E-02
+6.419E+03 0.0000 -0.1993 1.720E-27 9.564E-02
+6.457E+03 0.0000 -0.1992 1.712E-27 9.520E-02
+6.494E+03 0.0000 -0.1991 1.704E-27 9.476E-02
+6.531E+03 0.0000 -0.1990 1.696E-27 9.432E-02
+6.569E+03 0.0000 -0.1989 1.688E-27 9.389E-02
+6.607E+03 0.0000 -0.1989 1.681E-27 9.345E-02
+6.645E+03 0.0000 -0.1988 1.673E-27 9.302E-02
+6.683E+03 0.0000 -0.1987 1.665E-27 9.259E-02
+6.722E+03 0.0000 -0.1986 1.657E-27 9.216E-02
+6.761E+03 0.0000 -0.1985 1.650E-27 9.173E-02
+6.800E+03 0.0000 -0.1984 1.642E-27 9.130E-02
+6.839E+03 0.0000 -0.1983 1.634E-27 9.088E-02
+6.879E+03 0.0000 -0.1982 1.627E-27 9.046E-02
+6.918E+03 0.0000 -0.1981 1.619E-27 9.003E-02
+6.958E+03 0.0000 -0.1980 1.612E-27 8.961E-02
+6.998E+03 0.0000 -0.1979 1.604E-27 8.920E-02
+7.039E+03 0.0000 -0.1979 1.597E-27 8.878E-02
+7.079E+03 0.0000 -0.1978 1.589E-27 8.836E-02
+7.120E+03 0.0000 -0.1977 1.582E-27 8.795E-02
+7.161E+03 0.0000 -0.1976 1.574E-27 8.753E-02
+7.203E+03 0.0000 -0.1975 1.567E-27 8.712E-02
+7.244E+03 0.0000 -0.1974 1.559E-27 8.671E-02
+7.286E+03 0.0000 -0.1973 1.552E-27 8.630E-02
+7.328E+03 0.0000 -0.1972 1.545E-27 8.589E-02
+7.371E+03 0.0000 -0.1971 1.537E-27 8.548E-02
+7.413E+03 0.0000 -0.1970 1.530E-27 8.508E-02
+7.456E+03 0.0000 -0.1969 1.523E-27 8.467E-02
+7.499E+03 0.0000 -0.1968 1.516E-27 8.427E-02
+7.542E+03 0.0000 -0.1967 1.508E-27 8.387E-02
+7.586E+03 0.0000 -0.1966 1.501E-27 8.347E-02
+7.630E+03 0.0000 -0.1965 1.494E-27 8.307E-02
+7.674E+03 0.0000 -0.1964 1.487E-27 8.267E-02
+7.718E+03 0.0000 -0.1962 1.480E-27 8.228E-02
+7.762E+03 0.0000 -0.1961 1.473E-27 8.188E-02
+7.807E+03 0.0000 -0.1960 1.466E-27 8.149E-02
+7.852E+03 0.0000 -0.1959 1.458E-27 8.110E-02
+7.898E+03 0.0000 -0.1958 1.451E-27 8.071E-02
+7.943E+03 0.0000 -0.1957 1.444E-27 8.032E-02
+7.989E+03 0.0000 -0.1956 1.437E-27 7.993E-02
+8.035E+03 0.0000 -0.1955 1.431E-27 7.955E-02
+8.082E+03 0.0000 -0.1954 1.424E-27 7.916E-02
+8.128E+03 0.0000 -0.1953 1.417E-27 7.878E-02
+8.175E+03 0.0000 -0.1951 1.410E-27 7.840E-02
+8.222E+03 0.0000 -0.1950 1.403E-27 7.801E-02
+8.270E+03 0.0000 -0.1949 1.396E-27 7.763E-02
+8.318E+03 0.0000 -0.1948 1.389E-27 7.726E-02
+8.366E+03 0.0000 -0.1947 1.383E-27 7.688E-02
+8.414E+03 0.0000 -0.1946 1.376E-27 7.650E-02
+8.463E+03 0.0000 -0.1945 1.369E-27 7.613E-02
+8.511E+03 0.0000 -0.1943 1.362E-27 7.576E-02
+8.561E+03 0.0000 -0.1942 1.356E-27 7.538E-02
+8.610E+03 0.0000 -0.1941 1.349E-27 7.501E-02
+8.660E+03 0.0000 -0.1940 1.342E-27 7.464E-02
+8.710E+03 0.0000 -0.1938 1.336E-27 7.428E-02
+8.760E+03 0.0000 -0.1937 1.329E-27 7.391E-02
+8.810E+03 0.0000 -0.1936 1.323E-27 7.354E-02
+8.861E+03 0.0000 -0.1935 1.316E-27 7.318E-02
+8.913E+03 0.0000 -0.1933 1.309E-27 7.282E-02
+8.964E+03 0.0000 -0.1932 1.303E-27 7.245E-02
+9.016E+03 0.0000 -0.1931 1.296E-27 7.209E-02
+9.068E+03 0.0000 -0.1930 1.290E-27 7.173E-02
+9.120E+03 0.0000 -0.1928 1.284E-27 7.137E-02
+9.173E+03 0.0000 -0.1927 1.277E-27 7.101E-02
+9.226E+03 0.0000 -0.1926 1.271E-27 7.066E-02
+9.279E+03 0.0000 -0.1924 1.264E-27 7.030E-02
+9.333E+03 0.0000 -0.1923 1.258E-27 6.995E-02
+9.386E+03 0.0000 -0.1922 1.252E-27 6.959E-02
+9.441E+03 0.0000 -0.1921 1.245E-27 6.924E-02
+9.495E+03 0.0000 -0.1919 1.239E-27 6.889E-02
+9.550E+03 0.0000 -0.1918 1.233E-27 6.854E-02
+9.605E+03 0.0000 -0.1916 1.226E-27 6.819E-02
+9.661E+03 0.0000 -0.1915 1.220E-27 6.784E-02
+9.716E+03 0.0000 -0.1913 1.214E-27 6.750E-02
+9.772E+03 0.0000 -0.1912 1.208E-27 6.715E-02
+9.829E+03 0.0000 -0.1911 1.201E-27 6.681E-02
+9.886E+03 0.0000 -0.1909 1.195E-27 6.646E-02
+9.943E+03 0.0000 -0.1908 1.189E-27 6.612E-02
+1.000E+04 0.0000 -0.1906 1.183E-27 6.578E-02
diff --git a/dust_extinction/data/kext_albedo_WD_SMCbar_0.dat b/dust_extinction/data/kext_albedo_WD_SMCbar_0.dat
new file mode 100644
index 0000000..db1b28a
--- /dev/null
+++ b/dust_extinction/data/kext_albedo_WD_SMCbar_0.dat
@@ -0,0 +1,2444 @@
+Extinction, scattering, and absorption properties computed for the
+carbonaceous - silicate dust model of Weingartner & Draine (2001) and
+Li & Draine (2001).
+
+Model consists of mixture of carbonaceous grains, and amorphous
+silicate grains.  Carbonaceous grains are PAH-like when small, and
+graphite-like when large (see Li & Draine 2001).  Size distributions
+from Weingartner & Draine (2001).  PAH optical properties are from Li
+& Draine (2001).  Graphite and silicate optical properties from Draine
+& Lee (1984), Laor & Draine (1993), Weingartner & Draine (2001), and
+Li & Draine (2001).
+
+Grain size distribution: Weingartner & Draine (2001) model for
+"SMC bar" dust with C/H = b_C = 0 in two log-normal size
+distributions.
+
+The PAH/graphitic grains in the log-normal size distributions are
+assumed to be 50% neutral and 50% ionized.  The PAH/graphitic grains
+in the size distribution given by eq. (5,6) of Weingartner & Draine
+(2001) are assumed to be 100% ionized.
+
+Calculated by B.T. Draine, Princeton University, 2001.07.05
+
+References:
+Draine, B.T., & Lee, H.-M. 1984, "Optical Properties of Interstellar
+    Graphite and Silicate Grains", Astrophys. J., 285, 89-108
+Laor, A., & Draine, B.T. 1993, "Spectroscopic Constraints on the Properties
+    of Dust in Active Galactic Nuclei", Astrophys. J., 402, 441-468
+Li, A., & Draine, B.T. 2001, "Infrared Emission from Interstellar Dust. II.
+    The Diffuse Interstellar Medium", Astrophys. J., 554, 778-802
+Weingartner, J.C., & Draine, B.T. 2001, "Dust Grain-Size Distributions and 
+    Extinction in the Milky Way, LMC, and SMC", Astrophys. J., 548, 296-309
+
+Tabulated quantities:
+lambda  = wavelength in vacuo (micron) [2401 values from 1.e-2 to 1.e4 um]
+albedo  = (scattering cross section)/(extinction cross section)
+g       = <cos(theta)> for scattered light
+C_ext/H = extinction cross section per H nucleon (cm^2/H)
+K_abs   = absorption cross section per mass of dust (cm^2/gram)
+
+ lambda   albedo    g     C_ext/H    K_abs
+(micron)                  (cm^2/H)  (cm^2/g)
+--------- ------  ------ --------- ---------
+1.000E-02 0.3444  0.9861 1.729E-22 3.233E+04
+1.006E-02 0.3426  0.9860 1.733E-22 3.249E+04
+1.012E-02 0.3409  0.9859 1.736E-22 3.265E+04
+1.017E-02 0.3391  0.9857 1.740E-22 3.280E+04
+1.023E-02 0.3374  0.9856 1.744E-22 3.296E+04
+1.029E-02 0.3356  0.9854 1.748E-22 3.312E+04
+1.035E-02 0.3335  0.9853 1.750E-22 3.328E+04
+1.041E-02 0.3304  0.9852 1.751E-22 3.344E+04
+1.047E-02 0.3273  0.9852 1.751E-22 3.360E+04
+1.053E-02 0.3215  0.9852 1.745E-22 3.378E+04
+1.059E-02 0.3097  0.9855 1.726E-22 3.398E+04
+1.065E-02 0.3083  0.9853 1.730E-22 3.414E+04
+1.072E-02 0.3308  0.9873 1.520E-22 2.902E+04
+1.078E-02 0.3295  0.9872 1.526E-22 2.918E+04
+1.084E-02 0.3425  0.9865 1.562E-22 2.929E+04
+1.090E-02 0.3499  0.9861 1.586E-22 2.941E+04
+1.096E-02 0.3517  0.9858 1.598E-22 2.956E+04
+1.103E-02 0.3533  0.9855 1.610E-22 2.970E+04
+1.109E-02 0.3547  0.9852 1.621E-22 2.984E+04
+1.116E-02 0.3558  0.9850 1.632E-22 2.999E+04
+1.122E-02 0.3568  0.9847 1.642E-22 3.013E+04
+1.128E-02 0.3576  0.9845 1.652E-22 3.028E+04
+1.135E-02 0.3582  0.9842 1.662E-22 3.042E+04
+1.142E-02 0.3587  0.9839 1.671E-22 3.057E+04
+1.148E-02 0.3590  0.9837 1.680E-22 3.071E+04
+1.155E-02 0.3592  0.9834 1.688E-22 3.086E+04
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diff --git a/dust_extinction/grain_models.py b/dust_extinction/grain_models.py
index 0508234..485b302 100644
--- a/dust_extinction/grain_models.py
+++ b/dust_extinction/grain_models.py
@@ -3,16 +3,17 @@ from scipy.interpolate import interp1d
 import numpy as np
 
 from astropy.table import Table
+from astropy.modeling import InputParameterError
 
 from .helpers import _get_x_in_wavenumbers, _test_valid_x_range
 from .baseclasses import BaseExtModel
 
-__all__ = ["D03_MWRV31", "D03_MWRV40", "D03_MWRV55", "ZDA04_MWRV31"]
+__all__ = ["WD01", "D03", "ZDA04"]
 
 
-class D03_Base(BaseExtModel):
+class WD01(BaseExtModel):
     r"""
-    Draine (2003) Grain Model Base
+    Weingartner & Draine (2001) Grain Models
 
     Parameters
     ----------
@@ -24,13 +25,60 @@ class D03_Base(BaseExtModel):
 
     Notes
     -----
-    From Draine (2003, ARA&A, 41, 241; 2003, ApJ, 598, 1017).
-    Using Weingartner & Draine (2001, ApJ, 548, 296) size distributions
+    From Weingartner & Draine (2001, ApJ, 548, 296)
+
+    Example showing the possible curves
+
+    .. plot::
+        :include-source:
+
+        import numpy as np
+        import matplotlib.pyplot as plt
+        import astropy.units as u
+
+        from dust_extinction.grain_models import WD01
+
+        fig, ax = plt.subplots()
+
+        tmod = WD01()
+        possmodels = tmod.possnames.keys()
+
+        # generate the curves and plot them
+        lam = np.logspace(-2.0, 4.0, num=1000)
+        x = (1.0 / lam) / u.micron
+
+        for cmodel in possmodels:
+            # define the extinction model
+            ext_model = WD01(cmodel)
+            ax.plot(lam,ext_model(x),label=cmodel)
+
+        ax.set_xlabel(r'$\lambda$ [$\mu m$]')
+        ax.set_ylabel(r'$A(x)/A(V)$')
+
+        ax.set_xscale('log')
+        ax.set_yscale('log')
+
+        ax.legend(loc='best')
+        plt.show()
     """
 
-    x_range = [1e-4, 1e4]
+    x_range = [1e-4, 1e2]
+
+    possnames = {
+        "MWRV31": ("kext_albedo_WD_MW_3.1_60.dat", 3.1),
+        "MWRV40": ("kext_albedo_WD_MW_4.0B_40.dat", 4.0),
+        "MWRV55": ("kext_albedo_WD_MW_5.5B_30.dat", 5.5),
+        "LMCAvg": ("kext_albedo_WD_LMCavg_20.dat", 3.1),
+        "LMC2": ("kext_albedo_WD_LMC2_10.dat", 3.1),
+        "SMCBar": ("kext_albedo_WD_SMCbar_0.dat", 3.1),
+    }
 
-    def __init__(self, filename, **kwargs):
+    def __init__(self, modelname="MWRV31", **kwargs):
+
+        if modelname not in self.possnames.keys():
+            raise InputParameterError("modelname not recognized")
+        filename = self.possnames[modelname][0]
+        self.Rv = self.possnames[modelname][1]
 
         # get the tabulated information
         data_path = pkg_resources.resource_filename("dust_extinction", "data/")
@@ -39,29 +87,29 @@ class D03_Base(BaseExtModel):
             data_path + filename,
             format="ascii.fixed_width",
             header_start=None,
-            data_start=67,
+            data_start=41,
             names=("wave", "albedo", "g", "cext"),
-            col_starts=(0, 12, 19, 26),
-            col_ends=(11, 18, 25, 35),
+            col_starts=(0, 10, 18, 25),
+            col_ends=(9, 16, 24, 34),
         )
 
-        self.obsdata_x = 1.0 / a["wave"].data
+        self.data_x = 1.0 / a["wave"].data
 
         # normalized by wavelength closest to V band
-        sindxs = np.argsort(np.absolute(self.obsdata_x - 1.0 / 0.55))
+        sindxs = np.argsort(np.absolute(self.data_x - 1.0 / 0.55))
 
         # ext is A(lambda)/A(K)
         # A(K)/A(V) = 0.112 (F19, R(V) = 3.1)
-        self.obsdata_axav = a["cext"].data / a["cext"].data[sindxs[0]]
+        self.data_axav = a["cext"].data / a["cext"].data[sindxs[0]]
 
-        # accuracy of the observed data based on published table
-        self.obsdata_tolerance = 1e-6
+        # accuracy of the observed data based on calculations
+        self.data_tolerance = 1e-6
 
         super().__init__(**kwargs)
 
     def evaluate(self, in_x):
         """
-        D03 function
+        WD01 function
 
         Parameters
         ----------
@@ -87,14 +135,16 @@ class D03_Base(BaseExtModel):
         _test_valid_x_range(x, self.x_range, self.__class__.__name__)
 
         # define the function allowing for spline interpolation
-        f = interp1d(self.obsdata_x, self.obsdata_axav)
+        #   fill value needed to handle numerical issues at the edges
+        #   the x values has already been checked to be in range
+        f = interp1d(self.data_x, self.data_axav, fill_value="extrapolate")
 
         return f(x)
 
 
-class D03_MWRV31(D03_Base):
+class D03(BaseExtModel):
     r"""
-    Draine (2003) MW RV=3.1 Grain Model Extinction Curve
+    Draine (2003) Grain Models
 
     Parameters
     ----------
@@ -109,7 +159,7 @@ class D03_MWRV31(D03_Base):
     From Draine (2003, ARA&A, 41, 241; 2003, ApJ, 598, 1017).
     Using Weingartner & Draine (2001, ApJ, 548, 296) size distributions
 
-    Example showing the curve
+    Example showing the possible curves
 
     .. plot::
         :include-source:
@@ -118,18 +168,21 @@ class D03_MWRV31(D03_Base):
         import matplotlib.pyplot as plt
         import astropy.units as u
 
-        from dust_extinction.grain_models import D03_MWRV31
+        from dust_extinction.grain_models import D03
 
         fig, ax = plt.subplots()
 
-        # define the extinction model
-        ext_model = D03_MWRV31()
+        tmod = D03()
+        possmodels = tmod.possnames.keys()
 
         # generate the curves and plot them
         lam = np.logspace(-4.0, 4.0, num=1000)
         x = (1.0 / lam) / u.micron
 
-        ax.plot(1.0/x,ext_model(x),label='D03_MWRV31')
+        for cmodel in possmodels:
+            # define the extinction model
+            ext_model = D03(cmodel)
+            ax.plot(lam,ext_model(x),label=cmodel)
 
         ax.set_xlabel(r'$\lambda$ [$\mu m$]')
         ax.set_ylabel(r'$A(x)/A(V)$')
@@ -141,72 +194,86 @@ class D03_MWRV31(D03_Base):
         plt.show()
     """
 
-    Rv = 3.1
+    x_range = [1e-4, 1e4]
 
-    def __init__(self, **kwargs):
+    possnames = {
+        "MWRV31": ("kext_albedo_WD_MW_3.1_60_D03.dat", 3.1),
+        "MWRV40": ("kext_albedo_WD_MW_4.0A_40_D03.dat", 4.0),
+        "MWRV55": ("kext_albedo_WD_MW_5.5A_30_D03.dat", 5.5),
+    }
 
-        super().__init__("kext_albedo_WD_MW_3.1_60_D03.dat", **kwargs)
+    def __init__(self, modelname="MWRV31", **kwargs):
 
+        if modelname not in self.possnames.keys():
+            raise InputParameterError("modelname not recognized")
+        filename = self.possnames[modelname][0]
+        self.Rv = self.possnames[modelname][1]
 
-class D03_MWRV40(D03_Base):
-    r"""
-    Draine (2003) MW RV=4.0 Grain Model Extinction Curve
-
-    Parameters
-    ----------
-    None
-
-    Raises
-    ------
-    None
-
-    Notes
-    -----
-    From Draine (2003, ARA&A, 41, 241; 2003, ApJ, 598, 1017).
-    Using Weingartner & Draine (2001, ApJ, 548, 296) size distributions
+        # get the tabulated information
+        data_path = pkg_resources.resource_filename("dust_extinction", "data/")
 
-    Example showing the curve
+        a = Table.read(
+            data_path + filename,
+            format="ascii.fixed_width",
+            header_start=None,
+            data_start=67,
+            names=("wave", "albedo", "g", "cext"),
+            col_starts=(0, 12, 19, 26),
+            col_ends=(11, 18, 25, 35),
+        )
 
-    .. plot::
-        :include-source:
+        self.data_x = 1.0 / a["wave"].data
 
-        import numpy as np
-        import matplotlib.pyplot as plt
-        import astropy.units as u
+        # normalized by wavelength closest to V band
+        sindxs = np.argsort(np.absolute(self.data_x - 1.0 / 0.55))
 
-        from dust_extinction.grain_models import D03_MWRV40
+        # ext is A(lambda)/A(K)
+        # A(K)/A(V) = 0.112 (F19, R(V) = 3.1)
+        self.data_axav = a["cext"].data / a["cext"].data[sindxs[0]]
 
-        fig, ax = plt.subplots()
+        # accuracy of the observed data based on calculations
+        self.data_tolerance = 1e-6
 
-        # define the extinction model
-        ext_model = D03_MWRV40()
+        super().__init__(**kwargs)
 
-        # generate the curves and plot them
-        lam = np.logspace(-4.0, 4.0, num=1000)
-        x = (1.0 / lam) / u.micron
+    def evaluate(self, in_x):
+        """
+        D03 function
 
-        ax.plot(1.0/x,ext_model(x),label='D03_MWRV40')
+        Parameters
+        ----------
+        in_x: float
+           expects either x in units of wavelengths or frequency
+           or assumes wavelengths in wavenumbers [1/micron]
 
-        ax.set_xlabel(r'$\lambda$ [$\mu m$]')
-        ax.set_ylabel(r'$A(x)/A(V)$')
+           internally wavenumbers are used
 
-        ax.set_xscale('log')
-        ax.set_yscale('log')
+        Returns
+        -------
+        axav: np array (float)
+            A(x)/A(V) extinction curve [mag]
 
-        ax.legend(loc='best')
-        plt.show()
-    """
+        Raises
+        ------
+        ValueError
+           Input x values outside of defined range
+        """
+        x = _get_x_in_wavenumbers(in_x)
 
-    Rv = 4.0
+        # check that the wavenumbers are within the defined range
+        _test_valid_x_range(x, self.x_range, self.__class__.__name__)
 
-    def __init__(self, **kwargs):
+        # define the function allowing for spline interpolation
+        #   fill value needed to handle numerical issues at the edges
+        #   the x values has already been checked to be in range
+        f = interp1d(self.data_x, self.data_axav, fill_value="extrapolate")
 
-        super().__init__("kext_albedo_WD_MW_4.0A_40_D03.dat", **kwargs)
+        return f(x)
 
 
-class D03_MWRV55(D03_Base):
+class ZDA04(BaseExtModel):
     r"""
-    Draine (2003) MW RV=5.5 Grain Model Extinction Curve
+    Zubko, Dwek, & Arendt (2004) Grain Models
 
     Parameters
     ----------
@@ -218,10 +285,10 @@ class D03_MWRV55(D03_Base):
 
     Notes
     -----
-    From Draine (2003, ARA&A, 41, 241; 2003, ApJ, 598, 1017).
-    Using Weingartner & Draine (2001, ApJ, 548, 296) size distributions
+    BARE-GR-S model from Zubko, Dwek, & Arendt (2004, ApJS, 152, 211)
+    Calculated by K. Misselt using ZDA04 grain size distributions and compositions
 
-    Example showing the curve
+    Example showing the possible curves
 
     .. plot::
         :include-source:
@@ -230,18 +297,21 @@ class D03_MWRV55(D03_Base):
         import matplotlib.pyplot as plt
         import astropy.units as u
 
-        from dust_extinction.grain_models import D03_MWRV55
+        from dust_extinction.grain_models import ZDA04
 
         fig, ax = plt.subplots()
 
-        # define the extinction model
-        ext_model = D03_MWRV55()
+        tmod = ZDA04()
+        possmodels = tmod.possnames.keys()
 
         # generate the curves and plot them
-        lam = np.logspace(-4.0, 4.0, num=1000)
+        lam = np.logspace(-3.0, 4.0, num=1000)
         x = (1.0 / lam) / u.micron
 
-        ax.plot(1.0/x,ext_model(x),label='D03_MWRV55')
+        for cmodel in possmodels:
+            # define the extinction model
+            ext_model = ZDA04(cmodel)
+            ax.plot(lam,ext_model(x),label=cmodel)
 
         ax.set_xlabel(r'$\lambda$ [$\mu m$]')
         ax.set_ylabel(r'$A(x)/A(V)$')
@@ -253,62 +323,39 @@ class D03_MWRV55(D03_Base):
         plt.show()
     """
 
-    Rv = 5.5
-
-    def __init__(self, **kwargs):
-
-        super().__init__("kext_albedo_WD_MW_5.5A_30_D03.dat", **kwargs)
-
-
-class ZDA04_MWRV31(BaseExtModel):
-    r"""
-    Zubko, Dwek, Arendt Milky Way R(V)=3.1 Grain Model Extinction Curve
-
-    Parameters
-    ----------
-    None
-
-    Raises
-    ------
-    None
-
-    Notes
-    -----
-    BARE-GR-S model from Zubko, Dwek, & Arendt (2004, ApJS, 152, 211)
-    Calculated by K. Misselt using ZDA04 grain size distributions and compositions
-    """
-
     x_range = [1e-4, 1e3]
 
-    Rv = 3.1
+    possnames = {"BARE-GR-S": ("zubko2004_bare-gr-s_alam_av.dat", 3.1)}
+
+    def __init__(self, modelname="BARE-GR-S", **kwargs):
 
-    def __init__(self, **kwargs):
+        if modelname not in self.possnames.keys():
+            raise InputParameterError("modelname not recognized")
+        filename = self.possnames[modelname][0]
+        self.Rv = self.possnames[modelname][1]
 
         # get the tabulated information
         data_path = pkg_resources.resource_filename("dust_extinction", "data/")
 
-        a = Table.read(
-            data_path + "zubko2004_bare-gr-s_alam_av.dat",
-            format="ascii.basic",
-        )
+        a = Table.read(data_path + filename, format="ascii.basic",)
 
-        self.obsdata_x = 1.0 / a["lam[um]"].data
+        self.data_x = 1.0 / a["lam[um]"].data
 
         # normalized by wavelength closest to V band
-        sindxs = np.argsort(np.absolute(self.obsdata_x - 1.0 / 0.55))
+        sindxs = np.argsort(np.absolute(self.data_x - 1.0 / 0.55))
 
         # ext is A(lambda)/A(K)
         # A(K)/A(V) = 0.112 (F19, R(V) = 3.1)
-        self.obsdata_axav = a["A_lam/A_V"].data / a["A_lam/A_V"].data[sindxs[0]]
+        self.data_axav = a["A_lam/A_V"].data / a["A_lam/A_V"].data[sindxs[0]]
 
-        # accuracy of the observed data based on published table
-        self.obsdata_tolerance = 1e-6
+        # accuracy of the observed data based on calculations
+        self.data_tolerance = 1e-6
 
         super().__init__(**kwargs)
 
     def evaluate(self, in_x):
         """
-        ZDA04_MWRV31 function
+        ZDA04 function
 
         Parameters
         ----------
@@ -334,6 +381,8 @@ class ZDA04_MWRV31(BaseExtModel):
         _test_valid_x_range(x, self.x_range, self.__class__.__name__)
 
         # define the function allowing for spline interpolation
-        f = interp1d(self.obsdata_x, self.obsdata_axav)
+        #   fill value needed to handle numerical issues at the edges
+        #   the x values has already been checked to be in range
+        f = interp1d(self.data_x, self.data_axav, fill_value="extrapolate")
 
         return f(x)


Test patch:
diff --git a/dust_extinction/tests/helpers.py b/dust_extinction/tests/helpers.py
index 242d1e6..ddb45a8 100644
--- a/dust_extinction/tests/helpers.py
+++ b/dust_extinction/tests/helpers.py
@@ -24,12 +24,7 @@ from dust_extinction.averages import (
     GCC09_MWAvg,
     F11_MWGC,
 )
-from dust_extinction.grain_models import (
-    D03_MWRV31,
-    D03_MWRV40,
-    D03_MWRV55,
-    ZDA04_MWRV31,
-)
+from dust_extinction.grain_models import WD01, D03, ZDA04
 
 param_ave_models_Rv = [CCM89, O94, F99, F04, VCG04, GCC09, M14, F19]
 param_ave_models_Rv_fA = [G16]
@@ -47,7 +42,7 @@ ave_models = [
     GCC09_MWAvg,
     F11_MWGC,
 ]
-grain_models = [D03_MWRV31, D03_MWRV40, D03_MWRV55, ZDA04_MWRV31]
+grain_models = [WD01, D03, ZDA04]
 
 all_models = (
     param_ave_models_Rv
diff --git a/dust_extinction/tests/test_corvals_aves.py b/dust_extinction/tests/test_corvals_aves.py
index ab9fc98..bbdece5 100644
--- a/dust_extinction/tests/test_corvals_aves.py
+++ b/dust_extinction/tests/test_corvals_aves.py
@@ -2,11 +2,10 @@ import pytest
 import numpy as np
 import astropy.units as u
 
-# average and grain models behave the same
-from .helpers import ave_models, grain_models
+from .helpers import ave_models
 
 
-@pytest.mark.parametrize("model_class", ave_models + grain_models)
+@pytest.mark.parametrize("model_class", ave_models)
 def test_corvals(model_class):
     # instantiate extinction model
     tmodel = model_class()
@@ -23,7 +22,7 @@ def test_corvals(model_class):
         np.testing.assert_allclose(tmodel.evaluate(x), y, rtol=tol)
 
 
-@pytest.mark.parametrize("model_class", ave_models + grain_models)
+@pytest.mark.parametrize("model_class", ave_models)
 def test_extinguish_values_Av_or_Ebv(model_class):
     ext = model_class()
     x = np.arange(ext.x_range[0], ext.x_range[1]) / u.micron
diff --git a/dust_extinction/tests/test_corvals_grainmods.py b/dust_extinction/tests/test_corvals_grainmods.py
new file mode 100644
index 0000000..af37109
--- /dev/null
+++ b/dust_extinction/tests/test_corvals_grainmods.py
@@ -0,0 +1,41 @@
+import pytest
+import numpy as np
+import astropy.units as u
+
+from .helpers import grain_models
+
+
+@pytest.mark.parametrize("model_class", grain_models)
+def test_corvals(model_class):
+    # instantiate extinction model
+    tmodel = model_class()
+    # get the possible list of models
+    possmodels = tmodel.possnames.keys()
+
+    for cmodel in possmodels:
+        tmodel = model_class(cmodel)
+
+        # test array evaluation
+        x_vals = tmodel.data_x
+        y_vals = tmodel.data_axav
+        tol = tmodel.data_tolerance
+        np.testing.assert_allclose(tmodel(x_vals), y_vals, rtol=tol)
+
+
+@pytest.mark.parametrize("model_class", grain_models)
+def test_extinguish_values_Av_or_Ebv(model_class):
+    # just test the default model
+    ext = model_class()
+    x = np.arange(ext.x_range[0], ext.x_range[1]) / u.micron
+    cor_axav = ext(x)
+
+    # calculate the cor_vals in fractional units
+    Av = 1.0
+    cor_vals_av = np.power(10.0, -0.4 * (cor_axav * Av))
+    Ebv = 1.0
+    Av_ebv = Ebv * ext.Rv
+    cor_vals_ebv = np.power(10.0, -0.4 * cor_axav * Av_ebv)
+
+    # tests
+    np.testing.assert_equal(ext.extinguish(x, Av=Av), cor_vals_av)
+    np.testing.assert_equal(ext.extinguish(x, Ebv=Ebv), cor_vals_ebv)
diff --git a/dust_extinction/tests/test_warnings.py b/dust_extinction/tests/test_warnings.py
index cc73da4..628b564 100644
--- a/dust_extinction/tests/test_warnings.py
+++ b/dust_extinction/tests/test_warnings.py
@@ -12,6 +12,7 @@ from .helpers import (
     param_ave_models_Rv_fA,
     param_ave_models,
     ave_models,
+    grain_models,
 )
 
 
@@ -79,3 +80,10 @@ def test_extinguish_no_av_or_ebv(model):
     with pytest.raises(InputParameterError) as exc:
         ext.extinguish(ext.x_range[0])
     assert exc.value.args[0] == "neither Av or Ebv passed, one required"
+
+
+@pytest.mark.parametrize("model", grain_models)
+def test_possible_grain_model(model):
+    with pytest.raises(InputParameterError) as exc:
+        model("badmodename")
+    assert exc.value.args[0] == "modelname not recognized"