Substantial
changes in pressure can be measured fairly accurately by a simple
manometer: a U-shaped tube of glass containing a fluid of known density,
such as water.
One arm of the tube is
connected to the vessel containing gas under unknown pressure. If
the gas pressure is higher than atmospheric pressure, fluid moves
downward in that arm and upward in the other arm. The pressure is
equal to the difference in the height of the fluid in the alms multiplied
by the specific weight of the fluid. The height can be measured with
reasonable accuracy to within .5 millimeter. In the case of water
.5 millimeter is equal to .0014 pound per square inch.
By a simple modification
of the manometer the sensitivity of the instrument can be increased
by a factor of several thousand. Details of the modification are explained
by Kipling Adams, who is associated with the General RadioCompany
in West Concord, Mass. Adams writes:
"The sensitive manometer
consists of two cylindrical containers interconnected near the bottom
by a pair of tubes. One of them is a capillary made of glass or clear
plastic and therefore transparent. Each tube contains a stopcock.
The assembly is filled with fluid. The movement of the fluid is indicated
by a bubble of air trapped in the middle of the capillary.
"One cylinder is closed
at the top by a gastight lid containing a pipe nipple through which
the manometer is connected to the source of unknown pressure. The
top of the second cylinder is exposed to the air in the room. The
principle of the device is as simple as its construction. A difference
in pressure that acts on the surface of fluid in the containers causes
fluid to flow through the capillary toward the container of lesser
pressure, as is indicated by the movement of the bubble.
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Figure 1:
Figure 6: Elements of the manometer designed
by Kipling Adams
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"The dimensions are
not critical, but, they must be known as accurately as possible for
calibrating the instrument. For instance, assume that the cylindrical
containers have a diameter of five inches and that the capillary has
a bore of .05 inch. If we now apply a pressure of 36 millionths of
a pound per square inch to the surface of the water in the closed
container, the water level will fall .00.5 inch and will flow through
the transparent tube until the level rises an equal amount in the
opposite container. (A cubic inch of water weighs about .036 pound.)
The ratio of the cross-sectional area of the cylindrical containers
in this example is 10,000 times the cross-sectional area of the bore
of the capillary. The bubble will therefore move five inches toward
the left. Hence a bubble displacement of 1/8 inch indicates a change
in pressure of a millionth of a pound per square inch.
"A practical device
can be made with a pair of coffee cans, two brass stopcocks, some
rubber tubing and the capillary. Glass tubes with a bore of from .01
inch to several inches are available from distributors of scientific
supplies. Assemble the apparatus as indicated in the accompanying
illustration. Place it in operation by closing the stopcock connected
to the glass tube and opening the other stopcock. Fill the cans about
three-quarters full of water. When the levels have equalized, close
that stopcock and open the other one. With a medicine dropper add
a few drops to one reservoir until water pushes most of the air out
of the glass tube. A few drops added to the second reservoir will
bring the air bubble back to the center of the tube. If the reservoirs
are five inches in diameter, each drop will move the bubble about
1.5 inches in a tube with a bore of .05 inch.
"The multiplying factor
of 10,000 may prove to be too large for some measurements and the
pressure range too small. A reduction factor of, say, 100 may be required.
You can make this reduction in sensitivity by shrinking the effective
diameter of the open reservoir from five inches to .5 inch. Reducing
the diameter this substantially is not as difficult as it might seem.
You can accomplish it by putting a nonfloating cylinder 4.741 inches
in diameter in the open reservoir. This 'dividing' plug does not need
to be placed concentrically in the reservoir. It will work in any
position, provided that it does not block the outlet tubes and provided
also that the level of the water in the reservoir does not reach the
top or bottom of the plug.
"The instrument can
also be used as a highly sensitive tilt indicator. The 10,000-to-1
sensitivity figure applies to the liquid levels, so that raising one
reservoir from the balance position 10 millionths of an inch displaces
the bubble almost 1/16 inch. To demonstrate the sensitivity of the
device, place a piece of wood two feet long and two by four inches
in cross section on supports two feet apart. Stand one reservoir on
the center of the board and the other reservoir above one of the supports.
The weight of a finger placed on the board near the center will cause
the wood to bow downward about .0001 inch and will displace the bubble
.5 inch!"