Pyrometry: A Practical Treatise on the Measurement of High TemperaturesDarling, Charles R. (Charles Robert)
Science
Pyrometry: A Practical Treatise on the Measurement of High Temperatures
Darling, Charles R. (Charles Robert)
Pyrometry
=Practical Forms of Calorimetric Pyrometers.=—When required
to estimate the temperature of a muffle furnace or other laboratory
appliance, a sheet-copper vessel of about 1500 c.c. capacity may be
used. This should rest on wooden supports in a second similar vessel,
about 2 inches wider, which acts as a shield against radiation. A
cylinder of nickel about 1½ inches long, and 1¼ inches in diameter,
with a hole of ½-inch diameter in the centre, is suitable for test
purposes. This may conveniently be heated in a nickel crucible; and
when transferring to the water the crucible may be grasped with a pair
of tongs, and tilted so as to allow the cylinder to drop into the
water. When used in a tube furnace, a length of thin nickel wire may
be attached to the cylinder to enable withdrawal to be accomplished
rapidly, allowance being made for the weight of the heated wire. The
transfer should be accomplished as speedily as possible, to avoid
radiation errors. The figure to be used to represent the specific heat
of nickel may be obtained from the curve (fig. 65), when the range
to be measured is approximately known. The water equivalent of the
vessel and thermometer should be determined as follows:—Place in the
vessel one-half the quantity of cold water used in the experiment—say
750 c.c.—and note the temperature (_t_{1}_) after stirring with the
thermometer. Then add an equal quantity of water at a temperature
(_t_{2}_) about 10° higher than _t_{1}_ Mix thoroughly with the
thermometer, and note the temperature of the mixture (_t_{3}_). Check
results may be obtained by varying the proportions of cold and warm
water, the total quantity always being equal to that used for quenching
the hot nickel. If W_{1} = the weight of cold water, and W_{2} that of
the warm, the water equivalent (_x_) is obtained from the equation
W_{2} (_t_{2}_ - _t_{3}_) - W_{1}(_t_{3}_ - _t_{1}_)
_x_ = ─────────────────────────────────────────────────────
_t_{3}_ - _t_{1}_.
This figure represents the weight of water equal in thermal capacity to
the vessel, and in a pyrometric measurement is added to the weight of
water taken.
In industrial practice, it is desirable to dispense, if possible, with
the necessity for calculations, so that a reading may be taken by
an unskilled observer. The earliest form of calorimetric pyrometer,
patented by Byström in 1862, consisted of a lagged zinc vessel into
which a piece of platinum was dropped, and a table was provided from
which the temperature of the furnace could be read by noting the rise
in temperature of the water. The modern industrial form, made by Messrs
Siemens, will now be described.
[Illustration: FIG. 66.—SIEMENS’ CALORIMETRIC OR “WATER” PYROMETER.]
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