Scientific American Supplement, No. 1082, September 26, 1896 — John Shaqi
Scientific American Supplement, No. 1082, September 26, 1896Various
Science
Scientific American Supplement, No. 1082, September 26, 1896
Various
Science -- Periodicals
When measuring the area of such a surface as that inclosed by the
boundary line shown in Fig. 3, a point, A, is chosen somewhat near the
center of the figure; the exact position is, however, immaterial. From
the point, A, a line, AB, is drawn in any direction to the boundary;
the tracing point of the planimeter is now placed at A, with the
hatchet at X, Fig. 3, that is, with the instrument roughly square with
AB. The hatchet is now lightly pressed in order to mark its position
on the paper by making a slight dent, then leaving the hatchet free to
move as shown in Fig. 1, the tracing point is caused to traverse the
line, AB, and the boundary line in a clockwise direction, as shown by
the arrows, returning to A via AB. The hatchet will now be found to
have taken up a new position, Y, which must be marked by again
pressing the hatchet to make a slight dent in the paper. If the figure
under measurement be on a separate sheet of paper, the paper must now
be revolved about the point, A, through about 180 deg. (by eye), using
the tracing point of the instrument as a center, care being taken that
neither the point nor the hatchet be shifted while the paper is being
turned. The line, AB, will again be roughly at right angles to the
instrument, but in the reverse direction (see dotted lines in Fig. 3).
Again cause the tracing point to traverse the line, AB, and the
boundary line as before, but this time in a contra-clockwise
direction. The hatchet after this backward motion will take up the new
position, X1, which may or may not coincide with X; if not, prick a
central point between X and X1, as shown, then, of course, the
distance of this point from Y is the mean side shift of the hatchet;
this distance measured from the zero of the scale on the back of the
instrument is the area of the figure in square inches. The scale is
read in exactly the same manner as a geometrical scale on a drawing,
the whole numbers being read to the right of the zero and the decimals
to the left. The instrument does not profess to give results nearer
than one-tenth of a square inch.
In some cases on large maps, for example, the figure cannot be turned
round as indicated above; in that case the instrument itself must be
turned round through 180° and two fresh dents, X¹Y¹, obtained; the
area of the figure is then the mean of the two readings, XY and X¹Y¹.
When the area is large the instrument will move through a large angle,
and consequently, if square with AB to start with, it will be
considerably out of square at the finish. In such a case it is only
necessary to see that the mean position of the instrument is square
with AB.
By carefully examining the scale it will be observed (see Fig. 1) that
the divisions are not equal, but that they gradually increase from
zero upward; herein consists the improvement of this instrument over
the ordinary hatchet planimeter invented by Knudsen, of Copenhagen,
who shows in a pamphlet published by him that
Public-domain text, read in full here on John Shaqi.
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