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EXAMINATION OF RAIN GAUGE
Reference Number | 53. |
Date of
Examination | 1863, April
6. |
County | Sussex |
Name of Station | St. Leonards, Marina |
Owner and
Observer | J. C. Savery,
Esq. |
Construction of
Gauge | III. (Numerals
referring to a series of engravings). |
Maker's Name | Casella |
Time of Reading | Daily, 9 a.m. |
Height of Gauge above
ground | Level. |
Height of Gauge above sea
level | 31
ft. |
Diameters (that marked M =
mean) | 5.00, 5.02, 5.01,
5.00, M, 5.007. |
Equivalents of Water (Scale point /
Grains) | .1 / 500, .5 /
2510 |
Error at Scale-point specified in
previous column | -.001,
-.005 |
Remarks on position,
&c. | In yard at back of
Marina; very much sheltered by buildings on S.E., S., and
S.W. |
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The effect of these visits is varied, but uniformly
beneficial. Those who are subjected to them, are frankley
told of any departures from ordinary custom or established
rules; and the consciousness that "there's a chiel amang ye
takin' notes, and faith he'll print 'em," acts beneficially
on very many whom I can hardly hope ever to visit
personally. For it is seldom that more than twelve stations
a week can be visited - and at that rate which could hardly
be maintained - it would take two years incessant
work to visit them all; so, with fragments of time only
available, it will, indeed, be a lengthy process. However,
with nearly a sixth of the gauges tested, I adhere to my
motto, "nil desperandum." Probably, future
examinations will be yet more serviceable, because I have
recently designed the little instrument represented in the
following figure - the object may as easily be explained as
the modus operandi. The influence of trees or houses
on the indications of rain gauges depends obviously neither
on their height nor their distance, but on the relation of
one to the other - in other words, the suitablity of any
position for a rain gauge depends on the angle which is
subtended by the top of the surrounding objects, which I
have always held should never exceed 30°.
The altameter represented in fig. 1 is an extremely simple
instrument, depending on two infallible laws, (1) gravity,
and (2) the angles of incidence and reflection are equal. It
consists of a brass tube, 6 in. long, and three-quarters of
an inch in diameter; near the top are double gimbals (c), by
the outermost of which the instrument is suspended between
the fingers, when, of course, the body assumes
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