 | An image should appear at this position in the text. To use the entire page scan as a placeholder, edit this page and replace "{{missing image}}" with "{{raw image|Radio-activity.djvu/137}}". Otherwise, if you are able to provide the image then please do so. For guidance, see Wikisource:Image guidelines and Help:Adding images. |  |
Fig. 24.
If screens of various thickness are placed on the plate, it is observed that the plate is not appreciably affected within a certain distance from the active matter, and that this distance increases with the thickness of the screen. This distance is obviously equal to twice the radius of curvature of the path of the rays, which are just able to produce an impression through the screen.
These experiments show very clearly that the most deviable rays are those most readily absorbed by matter. By observations of this kind Becquerel has determined approximately the inferior limit of the value of HR for rays which are transmitted through different thicknesses of matter.
The results are given in the table below:
+-+-++
| | Thickness | Inferior limit |
| Substance | in mms. | of HR for |
| | |transmitted rays|
+-+-++
| Black paper | 0·065 | 650 |
| Aluminium | 0·010 | 350 |
| " | 0·100 | 1000 |
| " | 0·200 | 1480 |
| Mica | 0·025 | 520 |
| Glass | 0·155 | 1130 |
| Platinum | 0·030 | 1310 |
| Copper | 0·085 | 1740 |
| Lead | 0·130 | 2610 |
+-+-++
If e/m is a constant for all the rays, the value of HR is proportional to the velocity of the rays, and it follows from the table that the velocity of the rays which just produce an effect on the plate through ·13 mms. of lead is about 7 times that of the rays which
