Table I
Electric vector expansion coefficients B1, B3 for h1=1 and α=180° (normal incidence).
h2 | Re[B1] | Im[B1] | Re[B3] | Im[B3] |
---|
0.4 | 0.29722 | 0.08382 | −0.00004 | −0.00002 |
0.8 | 0.56842 | 0.25690 | 0.00006 | −0.00009 |
1.2 | 0.68227 | 0.52060 | 0.00190 | 0.00049 |
1.6 | 0.58410 | 0.71371 | 0.03447 | 0.00425 |
2.0 | 0.39327 | 0.73070 | 0.02091 | 0.01944 |
Table II
Square of absolute value of electric vector expansion coefficients A1, B1, as a function of the angle of incidence α for h1=1.
h2/α | −90° | −70° | −50° | −30° | −10° | 0° |
---|
0.4 | 0.48410 | 0.41548 | 0.25678 | 0.10106 | 0.01149 | 0 |
0.6 | 0.52128 | 0.44740 | 0.27652 | 0.10835 | 0.01237 | 0 |
0.8 | 0.55562 | 0.47689 | 0.29473 | 0.11550 | 0.01318 | 0 |
1.0 | 0.57540 | 0.49386 | 0.30522 | 0.11961 | 0.01365 | 0 |
1.2 | 0.57028 | 0.48945 | 0.30251 | 0.11854 | 0.01353 | 0 |
1.4 | 0.53733 | 0.46118 | 0.28503 | 0.11169 | 0.01275 | 0 |
1.6 | 0.48325 | 0.41477 | 0.25624 | 0.10045 | 0.01147 | 0 |
1.8 | 0.41975 | 0.36026 | 0.22265 | 0.08725 | 0.00996 | 0 |
2.0 | 0.35704 | 0.30644 | 0.18939 | 0.07422 | 0.00847 | 0 |
0.4 | 0.09546 | 0.08193 | 0.05063 | 0.01993 | 0.00226 | 0 |
0.6 | 0.21997 | 0.18880 | 0.11669 | 0.04572 | 0.00522 | 0 |
0.8 | 0.38873 | 0.33365 | 0.20621 | 0.08081 | 0.00922 | 0 |
1.0 | 0.57540 | 0.49386 | 0.30522 | 0.11961 | 0.01365 | 0 |
1.2 | 0.73718 | 0.63271 | 0.39104 | 0.15324 | 0.01749 | 0 |
1.4 | 0.83332 | 0.71463 | 0.44203 | 0.17322 | 0.01977 | 0 |
1.6 | 0.84780 | 0.72766 | 0.44972 | 0.17623 | 0.02012 | 0 |
1.8 | 0.79374 | 0.68125 | 0.42104 | 0.16499 | 0.01883 | 0 |
2.0 | 0.69851 | 0.59952 | 0.37053 | 0.14519 | 0.01657 | 0 |
Table III
Square of absolute value of electric vector expansion coefficients A2, B2 as a function of the angle of incidence α for h1=1.
h2/α | −90° | −70° | −50° | −30° | −10° | 0° |
---|
0.4 | 0 | 0.00059 | 0.00131 | 0.00096 | 0.00014 | 0 |
0.6 | 0 | 0.00060 | 0.00133 | 0.00097 | 0.00015 | 0 |
0.8 | 0 | 0.00061 | 0.00137 | 0.00100 | 0.00015 | 0 |
1.0 | 0 | 0.00064 | 0.00142 | 0.00104 | 0.00016 | 0 |
1.2 | 0 | 0.00067 | 0.00149 | 0.00109 | 0.00016 | 0 |
1.4 | 0 | 0.00070 | 0.00157 | 0.00115 | 0.00017 | 0 |
1.6 | 0 | 0.00075 | 0.00167 | 0.00122 | 0.00018 | 0 |
1.8 | 0 | 0.00080 | 0.00180 | 0.00131 | 0.00020 | 0 |
2.0 | 0 | 0.00087 | 0.00194 | 0.00142 | 0.00021 | 0 |
0.4 | 0 | 0.00002 | 0.00004 | 0.00003 | 0.00000 | 0 |
0.6 | 0 | 0.00009 | 0.00019 | 0.00014 | 0.00002 | 0 |
0.8 | 0 | 0.00027 | 0.00060 | 0.00044 | 0.00007 | 0 |
1.0 | 0 | 0.00064 | 0.00142 | 0.00104 | 0.00016 | 0 |
1.2 | 0 | 0.00128 | 0.00287 | 0.00210 | 0.00032 | 0 |
1.4 | 0 | 0.00230 | 0.00514 | 0.00376 | 0.00057 | 0 |
1.6 | 0 | 0.00378 | 0.00845 | 0.00618 | 0.00093 | 0 |
1.8 | 0 | 0.00580 | 0.01297 | 0.00948 | 0.00142 | 0 |
2.0 | 0 | 0.00840 | 0.01876 | 0.01372 | 0.00206 | 0 |
Table IV
Scattered intensity at infinity Ω1e(h1,α) for normal incidence (α=−90°) in Region 1.
h2/v | 0° | −10° | −20° | −30° | −40° | −50° | −60° | −70° | −80° | −90° |
---|
0.4 | 0 | 0.0147 | 0.0583 | 0.1289 | 0.2218 | 0.3289 | 0.4375 | 0.5321 | 0.5969 | 0.6200 |
0.6 | 0 | 0.0158 | 0.0628 | 0.1388 | 0.2389 | 0.3541 | 0.4711 | 0.5730 | 0.6427 | 0.6676 |
0.8 | 0 | 0.0169 | 0.0669 | 0.1479 | 0.2546 | 0.3777 | 0.5021 | 0.6107 | 0.6851 | 0.7116 |
1.0 | 0 | 0.0175 | 0.0693 | 0.1532 | 0.2636 | 0.3909 | 0.5200 | 0.6325 | 0.7095 | 0.7369 |
1.2 | 0 | 0.0173 | 0.0687 | 0.1518 | 0.2613 | 0.3874 | 0.5154 | 0.6268 | 0.7032 | 0.7303 |
1.4 | 0 | 0.0163 | 0.0647 | 0.1430 | 0.2462 | 0.3650 | 0.4856 | 0.5906 | 0.6625 | 0.6881 |
1.6 | 0 | 0.0147 | 0.0582 | 0.1286 | 0.2214 | 0.3283 | 0.4367 | 0.5312 | 0.5958 | 0.6189 |
1.8 | 0 | 0.0128 | 0.0506 | 0.1117 | 0.1923 | 0.2051 | 0.3793 | 0.4614 | 0.5176 | 0.5376 |
2.0 | 0 | 0.0108 | 0.0430 | 0.0950 | 0.1636 | 0.2425 | 0.3227 | 0.3924 | 0.4402 | 0.4572 |
Table V
Scattered intensity at infinity Ω2e(h2,α) for normal incidence (α=−90°) in Region 2.
h2/v | 0° | −10° | −20° | −30° | −40° | −50° | −60° | −70° | −80° | −90° |
---|
0.4 | 0 | 0.0072 | 0.0281 | 0.0603 | 0.1002 | 0.1434 | 0.1844 | 0.2183 | 0.2406 | 0.2484 |
0.6 | 0 | 0.0111 | 0.0433 | 0.0937 | 0.1572 | 0.2268 | 0.2941 | 0.3504 | 0.3879 | 0.4010 |
0.8 | 0 | 0.0147 | 0.0579 | 0.1264 | 0.2145 | 0.3132 | 0.4107 | 0.4938 | 0.5498 | 0.5696 |
1.0 | 0 | 0.0175 | 0.0693 | 0.1532 | 0.2637 | 0.3909 | 0.5200 | 0.6325 | 0.7095 | 0.7369 |
1.2 | 0 | 0.0187 | 0.0750 | 0.1682 | 0.2946 | 0.4450 | 0.6022 | 0.7426 | 0.8405 | 0.8757 |
1.4 | 0 | 0.0182 | 0.0738 | 0.1684 | 0.3012 | 0.4650 | 0.6420 | 0.8044 | 0.9199 | 0.9618 |
1.6 | 0 | 0.0163 | 0.0669 | 0.1557 | 0.2853 | 0.4515 | 0.6376 | 0.8133 | 0.9408 | 0.9876 |
1.8 | 0 | 0.0136 | 0.0568 | 0.1353 | 0.2547 | 0.4143 | 0.5999 | 0.7806 | 0.9144 | 0.9640 |
2.0 | 0 | 0.0109 | 0.0461 | 0.1125 | 0.2182 | 0.3658 | 0.5443 | 0.7235 | 0.8591 | 0.9100 |
Table VI
Electric vector transmission coefficient Te′ as a function of h2 and α h1=1.0.
h2/α | −90° | −70° | −50° | −30° | −10° | 0° |
---|
0.4 | 0.1931 | 0.1658 | 0.1025 | 0.0403 | 0.0046 | 0 |
0.6 | 0.3081 | 0.2644 | 0.1635 | 0.0641 | 0.0073 | 0 |
0.8 | 0.4304 | 0.3695 | 0.2285 | 0.0896 | 0.0102 | 0 |
1.0 | 0.5454 | 0.4682 | 0.2896 | 0.1136 | 0.0130 | 0 |
1.2 | 0.6326 | 0.5432 | 0.3361 | 0.1319 | 0.0151 | 0 |
1.4 | 0.6761 | 0.5802 | 0.3595 | 0.1412 | 0.0161 | 0 |
1.6 | 0.6739 | 0.5790 | 0.3588 | 0.1410 | 0.0161 | 0 |
1.8 | 0.6372 | 0.5478 | 0.3399 | 0.1338 | 0.0153 | 0 |
2.0 | 0.5818 | 0.5005 | 0.3112 | 0.1228 | 0.0141 | 0 |
Table VII
Electric vector backscatter coefficient Re′ as a function of h2 and g for h1=1.0.
h2/α | −90° | −70° | −50° | −30° | −10° | 0z |
---|
0.4 | 0.4588 | 0.3940 | 0.2437 | 0.0960 | 0.0109 | 0 |
0.6 | 0.4941 | 0.4242 | 0.2624 | 0.1029 | 0.0118 | 0 |
0.8 | 0.5266 | 0.4522 | 0.2796 | 0.1097 | 0.0125 | 0 |
1.0 | 0.5454 | 0.4682 | 0.2896 | 0.1136 | 0.0130 | 0 |
1.2 | 0.5406 | 0.4641 | 0.2870 | 0.1126 | 0.0129 | 0 |
1.4 | 0.5093 | 0.4373 | 0.2705 | 0.1061 | 0.0121 | 0 |
1.6 | 0.4580 | 0.3933 | 0.2432 | 0.0955 | 0.0109 | 0 |
1.8 | 0.3978 | 0.3416 | 0.2114 | 0.0830 | 0.0095 | 0 |
2.0 | 0.3384 | 0.2906 | 0.1799 | 0.0706 | 0.0081 | 0 |
Table VIII
Scattered intensity at infinity Ω1m(h1,α) for normal incidence (α=−90°) in Region 1.
h2/v | 0° | −10° | −20° | −30° | −40° | −50° | −60° | −70° | −80° | −90° |
---|
0.4 | 0.0160 | 0.0162 | 0.0170 | 0.0182 | 0.0198 | 0.0216 | 0.0234 | 0.0249 | 0.0259 | 0.0263 |
0.6 | 0.0866 | 0.0880 | 0.0921 | 0.0987 | 0.1072 | 0.1169 | 0.1266 | 0.1349 | 0.1406 | 0.1426 |
0.8 | 0.2460 | 0.2500 | 0.2617 | 0.2803 | 0.3046 | 0.3321 | 0.3595 | 0.3832 | 0.3993 | 0.4049 |
1.0 | 0.4822 | 0.4899 | 0.5128 | 0.5494 | 0.5969 | 0.6507 | 0.7046 | 0.7509 | 0.7824 | 0.7936 |
1.2 | 0.7504 | 0.7625 | 0.7981 | 0.8551 | 0.9290 | 1.013 | 1.097 | 1.169 | 1.218 | 1.235 |
1.4 | 1.007 | 1.023 | 1.071 | 1.147 | 1.246 | 1.359 | 1.471 | 1.568 | 1.634 | 1.657 |
1.6 | 1.225 | 1.245 | 1.303 | 1.396 | 1.517 | 1.654 | 1.791 | 1.909 | 1.989 | 2.017 |
1.8 | 1.386 | 1.409 | 1.474 | 1.580 | 1.716 | 1.871 | 2.026 | 2.159 | 2.250 | 2.282 |
2.0 | 1.528 | 1.553 | 1.626 | 1.742 | 1.892 | 2.063 | 2.234 | 2.380 | 2.480 | 2.516 |
Table IX
Scattered intensity at infinity Ω2m(h2,α) for normal incidence (α=−90°) in Region 2.
h2/v | 0° | −10° | −20° | −30° | −40° | −50° | −60° | −70° | −80° | −90° |
---|
0.4 | 2.403 | 2.409 | 2.426 | 2.452 | 2.484 | 2.519 | 2.552 | 2.579 | 2.597 | 2.603 |
0.6 | 1.547 | 1.555 | 1.580 | 1.619 | 1.668 | 1.720 | 1.771 | 1.814 | 1.842 | 1.851 |
0.8 | 0.9027 | 0.9118 | 0.9384 | 0.9802 | 1.034 | 1.092 | 1.150 | 1.199 | 1.231 | 1.243 |
1.0 | 0.4822 | 0.4999 | 0.5128 | 0.5494 | 0.5969 | 0.6507 | 0.7046 | 0.7509 | 0.7824 | 0.7936 |
1.2 | 0.2413 | 0.2470 | 0.2641 | 0.2921 | 0.3293 | 0.3726 | 0.4172 | 0.4564 | 0.4835 | 0.4932 |
1.4 | 0.1155 | 0.1194 | 0.1310 | 0.1505 | 0.1773 | 0.2095 | 0.2436 | 0.2745 | 0.2962 | 0.3040 |
1.6 | 0.0538 | 0.0562 | 0.0637 | 0.0765 | 0.0947 | 0.1175 | 0.1425 | 0.1657 | 0.1824 | 0.1885 |
1.8 | 0.0245 | 0.0259 | 0.0314 | 0.0385 | 0.0504 | 0.0659 | 0.0835 | 0.1005 | 0.1129 | 0.1175 |
2.0 | 0.0114 | 0.0122 | 0.0150 | 0.0201 | 0.0279 | 0.0386 | 0.0512 | 0.0637 | 0.0731 | 0.0766 |
Table X
Magnetic vector transmission coefficient Tm′ as a function of h2 and α for h1=1.0.
h2/α | −90° | −70° | −50° | −30° | −10° | 0° |
---|
0.4 | 3.931 | 3.755 | 3.340 | 2.915 | 2.664 | 2.631 |
0.6 | 2.665 | 2.556 | 2.299 | 2.035 | 1.878 | 1.857 |
0.8 | 1.677 | 1.611 | 1.484 | 1.319 | 1.228 | 1.216 |
1.0 | 0.9906 | 0.9595 | 0.8851 | 0.8071 | 0.7598 | 0.7536 |
1.2 | 0.5636 | 0.5498 | 0.5161 | 0.4801 | 0.4578 | 0.4548 |
1.4 | 0.3161 | 0.3111 | 0.2985 | 0.2843 | 0.2752 | 0.2739 |
1.6 | 0.1780 | 0.1770 | 0.1743 | 0.1704 | 0.1676 | 0.1672 |
1.8 | 0.0987 | 0.0996 | 0.1013 | 0.1022 | 0.1023 | 0.1023 |
2.0 | 0.0601 | 0.0613 | 0.0638 | 0.0657 | 0.0666 | 0.0667 |
Table XI
Magnetic vector backscatter coefficient Rm′ as a function of h2 and α for h1=1.0.
h2/α | −90° | −70° | −50° | −30° | −10° | 0° |
---|
0.4 | 0.0328 | 0.0330 | 0.0333 | 0.0334 | 0.0332 | 0.0332 |
0.6 | 0.1780 | 0.1749 | 0.1678 | 0.1596 | 0.1544 | 0.1537 |
0.8 | 0.5055 | 0.4921 | 0.4598 | 0.4255 | 0.4044 | 0.4016 |
1.0 | 0.9906 | 0.9595 | 0.8851 | 0.8071 | 0.7598 | 0.7536 |
1.2 | 1.542 | 1.490 | 1.365 | 1.236 | 1.158 | 1.148 |
1.4 | 2.069 | 1.997 | 1.825 | 1.647 | 1.540 | 1.526 |
1.6 | 2.518 | 2.430 | 2.220 | 2.001 | 1.870 | 1.853 |
1.8 | 2.848 | 2.750 | 2.515 | 2.270 | 2.123 | 2.104 |
2.0 | 3.140 | 3.026 | 2.776 | 2.508 | 2.347 | 2.326 |