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
COMPARISON OF GAS AND PLATINUM SCALES.
δ = 1·5.
▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬┬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬┬▬▬▬▬▬▬▬▬▬▬▬▬
Platinum Thermometer│Air Thermometer Reading│ Difference
Reading (Pt.). │ _t_ (deg. C.). │(_t_ ▬ Pt.).
▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬┼▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬┼▬▬▬▬▬▬▬▬▬▬▬▬
-100 │ -97·1 │ +2·9
│ │
0 │ 0 │ 0
50 │ 49·6 │ -0·04
100 │ 100 │ 0
200 │ 203·1 │ 3·1
300 │ 309·8 │ 9·8
│ │
400 │ 420·2 │ 20·2
500 │ 534·9 │ 34·9
600 │ 654·4 │ 54·4
700 │ 779·4 │ 79·4
800 │ 910·7 │ 110·7
│ │
900 │ 1049·4 │ 149·4
1000 │ 1197·0 │ 197·0
1100 │ 1355·0 │ 255·0
1200 │ 1526·7 │ 326·7
1300 │ 1716·0 │ 416·0
▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬┴▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬▬┴▬▬▬▬▬▬▬▬▬▬▬▬
=Terms used in Resistance Pyrometry.=—Following on the researches
of Callendar and others, certain terms relating to resistance
pyrometers have come into use, and will now be defined.
(1) _The Fundamental Interval_ is the increase in resistance between
0° C. and 100° C, or R_{100}-R_{0}. It should be remembered that the
increases between 200° and 300°, or 800° and 900°, all temperatures
being taken on the gas scale, differ from the fundamental increase.
(2) _The Fundamental Coefficient_ is that fraction of the resistance
at 0° C. by which it increases per degree between 0° and 100°, on the
average, or
(R_{100} - R_{0})
───────────────── .
(R_{0} × 100)
This figure is in reality the average temperature coefficient between
0° and 100°. For pure platinum the value is or 1/260 or 0·003846.
(3) _The Fundamental Zero_ is the temperature, on the platinum scale,
at which the resistance would vanish; it is evidently the reciprocal of
(2), prefaced by a minus sign, or
(R_{0} × 100)
─ ───────────────── .
(R_{100} - R_{0})
For pure platinum this temperature would be -260_p_, since it is
assumed that the average increase or decrease per degree holds
throughout; that is, for every degree the metal is cooled the loss of
resistance is taken to be 1/260 the resistance at 0°. Hence at -260_p_
the resistance, on this assumption, would vanish.
Public-domain text, read in full here on John Shaqi.
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