|
|
|
| |
 Volume 1  |
 23 Mar. 1876
  |
 Page 70 
TD>
| | |
|
|
|
as to cause one corner to dip into the water as in Fig 4. Sound just
about as loud as before. No sensible difference.
- In the course of these experiments it was observed that the
attraction of the platinum for the liquid caused the liquid to rise
considerably above the level of the water as at P Fig 5 - so that the
platinum was really too deeply immersed and its vibration therefore
did not make so much difference in the resistance of the liquid as
if it only touched the surface of the liquid.
- The sides SS' of the platinum foil (Fig 5) were then slightly
oiled but the edge P was left untouched. There was then a repulsion
between the sides SS' and the liquid but an attraction between the
water and P.
The result was that the sound audible from
|
|
|
| |
 Volume 1  |
 23 Mar. 1876
  |
 Page 70 
TD>
| | |
|
|
|