_/_
F/2,0 F=100,000 mm (30,0°)
[ f/2,0 f=98,612 mm (30,0°) ]
_/_
F/2,0 F=100,000 mm (30,0°)
[ f/2,0 f=98,612 mm (30,0°) ]
N° |
Rayon |
Indice d |
Constringence |
Épaisseur |
0 |
air | ***** |
***** | |
1 |
76,500 | 1,61000 |
53,3 |
8,100 |
2 |
394,800 | air |
***** |
0,500 |
3 |
40,100 | 1,61500 |
56,1 |
15,000 |
4 |
103,500 | air |
***** |
0,100 |
5 |
104,500 | 1,61340 |
36,9 |
4,300 |
6 |
25,750 | air |
***** |
22,000 |
7 |
-31,600 | 1,64690 |
33,7 |
4,500 |
8 |
49,500 | air |
***** |
0,150 |
9 |
50,000 | 1,64370 |
48,3 |
15,700 |
10 |
-41,650 | air |
***** |
0,500 |
11 |
140,000 | 1,62340 |
56,3 |
8,100 |
12 |
-101,000 | air |
***** |
o3o-4k4j |
no dioptre diaphragme : 6 | Calcul n° 927
| |||
| Commentaire : GB 0 427 008 | ||||
| Inventeur : H. Lee | Maison : Kapella | Date : 1935 | 111/111 | |