Submarine Appliances And Their Uses
Deep Sea Diving, &c., &c.
Forfatter: R. H. Davis
År: 1911
Forlag: Siebe, Gorman & Co., Ltd.
Sted: London
Sider: 183
UDK: 626.02
A Diving Manual
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T riewald’s
Bell.
Fig, 91.
In 1728, Martin Triewald, a Swedish
military officer, contrived a diving bell of
a lighter and less expensive character than
Halley’s. This bell, as shown in Fig. 91,
was made of copper, tinned on the inside,
and was sunk by the lead weights (W W)
suspended round the mouth. The iron plate
(E) on which the diver stood was suspended
by chains (F F) at such a distance from the
bottom of the bell that, when he stood up-
right, his head reached just above the water
in the bell, where he had the advantage of
the coolest air. A spiral tube was fitted, by
which a diver inside the bell could inhale
the cooler and fresher air at the bottom
through a mouthpiece (M). Air was sup-
plied to this bell in the same way as Halley’s.
Charles Spalding introduced an improvement on Halley’s bell, the ob-
ject being to make it more portable, safer to handle, and to allow the clivers to have
control over it. In shape the bell was like
into a separate chamber by the watertight
partition (E F). The bell was weighted
with slabs of lead (D I)) hung from hooks
(S S) to keep it perpendicular in the water,
but these weights were not sufficient to sink
the bell without the addition of the balance
weight (W), which was hung from the centre
ot the bell by pulley blocks, and allowed to
reach down some distance below the bottom
of the bell. By lowering this weight to the
bottom, the bell, being thus relieved of a
weight of about 3 cwt., immediately rises,
and any strain on the suspension rope, or
danger of being capsized by any obstacle in
its descent, are thus avoided. By means of
cocks (G L), water or air may be admitted
to the upper chamber (P), so that the bell
may be made to sink or rise in the water at
pleasure. As in the case of Halley’s bell,
fresh air was supplied by lowering barrels.
(See Fig. 92.)
Halley’s, but the upper part (P) was formed
Fig. 92.