dlug_fali [nm] |
transm[%] |
E |
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385 |
9 |
3,21974025974026 |
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3,220 |
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390 |
13 |
3,17846153846154 |
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3,178 |
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395 |
18 |
3,13822784810127 |
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3,138 |
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400 |
23 |
3,099 |
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3,099 |
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405 |
28 |
3,06074074074074 |
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3,061 |
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410 |
34 |
3,02341463414634 |
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3,023 |
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415 |
40 |
2,98698795180723 |
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420 |
45 |
2,95142857142857 |
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425 |
50 |
2,91670588235294 |
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430 |
55 |
2,88279069767442 |
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435 |
61 |
2,84965517241379 |
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440 |
65 |
2,81727272727273 |
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445 |
68 |
2,78561797752809 |
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450 |
71 |
2,75466666666667 |
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455 |
74 |
2,7243956043956 |
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460 |
77 |
2,69478260869565 |
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465 |
79 |
2,6658064516129 |
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470 |
80 |
2,63744680851064 |
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475 |
81,5 |
2,60968421052632 |
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480 |
81 |
2,5825 |
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485 |
82 |
2,55587628865979 |
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490 |
85 |
2,52979591836735 |
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495 |
87,5 |
2,50424242424242 |
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500 |
89,5 |
2,4792 |
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505 |
89 |
2,45465346534653 |
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510 |
88 |
2,43058823529412 |
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515 |
86 |
2,40699029126214 |
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520 |
86,5 |
2,38384615384615 |
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525 |
87 |
2,36114285714286 |
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530 |
89 |
2,3388679245283 |
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535 |
91,5 |
2,31700934579439 |
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540 |
94 |
2,29555555555556 |
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545 |
93 |
2,27449541284404 |
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550 |
92,5 |
2,25381818181818 |
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555 |
90 |
2,23351351351351 |
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560 |
89 |
2,21357142857143 |
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565 |
88 |
2,19398230088496 |
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570 |
88 |
2,17473684210526 |
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575 |
90 |
2,15582608695652 |
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580 |
91 |
2,13724137931034 |
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585 |
94,5 |
2,11897435897436 |
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590 |
96,5 |
2,10101694915254 |
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595 |
95,5 |
2,08336134453782 |
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600 |
95 |
2,066 |
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605 |
92,5 |
2,04892561983471 |
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610 |
91,5 |
2,03213114754098 |
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615 |
88,5 |
2,01560975609756 |
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620 |
88 |
1,99935483870968 |
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625 |
87,5 |
1,98336 |
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|
630 |
88 |
1,96761904761905 |
|
|
Tmax |
Emax |
Tmim |
Emin |
|
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|
|
Współczynnik załamania podłoża szklanego |
|
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|
635 |
90 |
1,95212598425197 |
|
|
97 |
1,6638926 |
86 |
1,5892308 |
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|
640 |
92 |
1,936875 |
|
|
97 |
1,8925191 |
89 |
1,7708571 |
|
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|
Obliczanie współczynnika załamania n. |
|
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|
645 |
94 |
1,92186046511628 |
|
|
96,5 |
2,1010169 |
87,5 |
1,98336 |
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|
650 |
96 |
1,90707692307692 |
|
|
94 |
2,2955556 |
88 |
2,1747368 |
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|
655 |
97 |
1,89251908396947 |
|
|
89,5 |
2,4792 |
86 |
2,4069903 |
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|
660 |
96 |
1,87818181818182 |
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|
81 |
2,5825 |
|
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665 |
95,5 |
1,86406015037594 |
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670 |
94 |
1,85014925373134 |
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675 |
93,5 |
1,83644444444444 |
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680 |
90,5 |
1,82294117647059 |
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685 |
90 |
1,80963503649635 |
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690 |
89,5 |
1,79652173913043 |
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695 |
89 |
1,78359712230216 |
|
|
dlug |
745,000007813004 |
654,999994451839 |
590,00001380284 |
539,999989545015 |
500 |
|
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|
700 |
89 |
1,77085714285714 |
|
|
E |
1,6638926 |
1,8925191 |
2,1010169 |
2,2955556 |
2,4792 |
|
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|
|
705 |
90 |
1,75829787234043 |
|
|
Tmax |
97 |
97 |
96,5 |
94 |
89,5 |
|
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|
|
710 |
91 |
1,74591549295775 |
|
|
Tmin |
88 |
88 |
88,5 |
87 |
84,5 |
suma |
|
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|
715 |
93 |
1,73370629370629 |
|
|
n |
1,79942 |
1,79942 |
1,77353 |
1,75525 |
1,70926 |
8,83688 |
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|
720 |
94 |
1,72166666666667 |
|
|
nsred |
1,767376 |
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725 |
95,5 |
1,70979310344828 |
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730 |
96,5 |
1,69808219178082 |
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735 |
96,5 |
1,6865306122449 |
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740 |
97 |
1,67513513513514 |
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745 |
97 |
1,66389261744966 |
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750 |
95 |
1,6528 |
|
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755 |
94 |
1,64185430463576 |
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760 |
92 |
1,63105263157895 |
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765 |
90 |
1,62039215686275 |
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770 |
89 |
1,60987012987013 |
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775 |
86,5 |
1,59948387096774 |
|
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|
|
Korzystając z relacji |
|
|
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|
|
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|
|
|
780 |
86 |
1,58923076923077 |
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lamb |
1 |
2 |
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|
dlug |
590 |
655 |
|
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d |
1681,98 |
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Obliczanie współczynników odbicia światła: |
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na granicy powietrze - warstwa |
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na granicy warstwa - szkło |
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1,381 |
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1,162 |
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0,969 |
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0,823 |
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0,706 |
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0,07689 |
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0,590 |
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0,00566 |
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Obliczanie współczynnika absorbcji dla kilku energii |
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E |
T[%] |
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alfa*E |
m=1/2 |
m=3/2 |
m=2 |
m=3 |
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e |
1_2 |
3_2 |
2 |
3 |
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1,38067 |
3,21974025974026 |
9 |
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4,44539878441558 |
19,7615703524836 |
2,70358783897266 |
2,10841143622766 |
1,64425905470296 |
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3,220 |
19,762 |
2,704 |
2,108 |
1,644 |
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390 |
1,16205 |
3,17846153846154 |
13 |
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3,69353123076923 |
13,6421729526677 |
2,38943112763705 |
1,92185619409186 |
1,54577848595361 |
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3,178 |
13,642 |
2,389 |
1,922 |
1,546 |
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395 |
0,96857 |
3,13822784810127 |
18 |
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3,03959334683544 |
9,23912771412629 |
2,09834546276998 |
1,74344295772344 |
1,44856669255163 |
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3,138 |
9,239 |
2,098 |
1,743 |
1,449 |
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400 |
0,822836 |
3,099 |
23 |
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2,549968764 |
6,50234069737569 |
1,86647956893594 |
1,5968621618662 |
1,36619162965374 |
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3,099 |
6,502 |
1,866 |
1,597 |
1,366 |
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405 |
0,705884 |
3,06074074074074 |
28 |
|
2,16052791703704 |
4,6678808802964 |
1,67124423276956 |
1,46987343572059 |
1,29276611680906 |
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3,061 |
4,668 |
1,671 |
1,470 |
1,293 |
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410 |
0,590451 |
3,02341463414634 |
34 |
|
1,78517819414634 |
3,18686118485559 |
1,47159300749313 |
1,33610560740772 |
1,21309233263306 |
|
3,023 |
3,187 |
1,472 |
1,336 |
1,213 |
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Wykresy zależności |
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dla czterech rodzajów przejść |
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Przejście |
m |
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proste dozwolone |
1 / 2 |
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proste wzbronione |
3 / 2 |
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skośne dozwolone |
2 |
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skośne wzbronione |
3 |
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Wartość przerwy energetycznej odczytujemy z wykresu jako przecięcie się prostej przechodzącej przez większość punktów z osią Ox |
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