Reflection Moments R0, R1, and R2
B.3
For light incident on a medium with a greater index of refraction, no
critical angle exists. Consequently, the Equations (B.10)-(B.12) are
straightforward numerical integrals in which theta varies from 0 to
.
When light travels into a less dense medium, a critical angle
exists and the equation for calculating R0, R1, and R2 must be
modified. Since
when
,
R0 becomes
 |
(B24) |
so
 |
(B25) |
where
and
.
Similarly, the other two
moments become
 |
(B26) |
and
 |
(B27) |
Depending on the index of refraction ratio, either Equations (B.10)-(B.12)
or (B.25)-(B.27) were used to numerically evaluate the reflection moments.
An adaptive eighth-order quadrature algorithm which yields numerical
results accurate to any specified tolerance [15] was
implemented. In the table below the accuracy is .
Values for
R0 and R2 do not exist in the literature, however R1 values were
identical to those of Orchard [46] and Ryde [53,54].
Table B.1:
The Fresnel reflection moments R0, R1, and R2. Light is
incident from a medium with an index of refraction of ni and
transmitted into a medium with index nt. The moments in this table are
accurate to 0.001.
 |
R0 |
R1 |
R2 |
| 0.50 |
0.260 |
0.161 |
0.134 |
| 0.55 |
0.241 |
0.137 |
0.108 |
| 0.60 |
0.224 |
0.116 |
0.087 |
| 0.65 |
0.207 |
0.097 |
0.068 |
| 0.70 |
0.190 |
0.081 |
0.053 |
| 0.75 |
0.173 |
0.066 |
0.040 |
| 0.80 |
0.156 |
0.053 |
0.029 |
| 0.85 |
0.136 |
0.040 |
0.019 |
| 0.90 |
0.113 |
0.027 |
0.011 |
| 0.95 |
0.081 |
0.015 |
0.004 |
| 1.00 |
0.001 |
0.000 |
0.000 |
| 1.05 |
0.324 |
0.107 |
0.036 |
| 1.10 |
0.440 |
0.195 |
0.089 |
| 1.15 |
0.518 |
0.271 |
0.144 |
| 1.20 |
0.578 |
0.337 |
0.199 |
| 1.25 |
0.626 |
0.395 |
0.252 |
| 1.30 |
0.665 |
0.445 |
0.301 |
| 1.35 |
0.698 |
0.490 |
0.347 |
| 1.40 |
0.726 |
0.530 |
0.390 |
| 1.45 |
0.750 |
0.565 |
0.429 |
| 1.50 |
0.771 |
0.597 |
0.465 |
| 1.55 |
0.789 |
0.626 |
0.499 |
| 1.60 |
0.805 |
0.651 |
0.529 |
| 1.65 |
0.820 |
0.675 |
0.558 |
| 1.70 |
0.833 |
0.696 |
0.584 |
| 1.75 |
0.845 |
0.716 |
0.608 |
| 1.80 |
0.855 |
0.733 |
0.631 |
| 1.85 |
0.864 |
0.749 |
0.652 |
| 1.90 |
0.873 |
0.764 |
0.671 |
| 1.95 |
0.881 |
0.778 |
0.689 |
| 2.00 |
0.888 |
0.791 |
0.705 |
|
|