scholarly journals A thin-film platinum resistance thermometer for use at low temperatures and in high magnetic fields.

1986 ◽  
Vol 21 (6) ◽  
pp. 334-338
Author(s):  
Tomiyoshi HARUYAMA ◽  
Ryozo YOSHIZAKI
Keyword(s):  
Thin Film ◽  
Magnetic Fields ◽  
Low Temperatures ◽  
Platinum Resistance Thermometer ◽  
Platinum Resistance ◽  
High Magnetic Fields ◽  
Resistance Thermometer

Thin film platinum resistance thermometer for measurements in high magnetic fields

Cryogenics ◽  
1990 ◽  
Vol 30 (4) ◽  
pp. 348-350 ◽  
Author(s):  
D.A. Dimitrov ◽  
B.M. Terzijska ◽  
V. Guevezov ◽  
V.T. Kovachev
Keyword(s):  
Thin Film ◽  
Magnetic Fields ◽  
Platinum Resistance Thermometer ◽  
Platinum Resistance ◽  
High Magnetic Fields ◽  
Resistance Thermometer

Thin-film alternating current nanocalorimeter for low temperatures and high magnetic fields

2005 ◽  
Vol 76 (4) ◽  
pp. 043906 ◽  
Author(s):  
A. A. Minakov ◽  
S. B. Roy ◽  
Y. V. Bugoslavsky ◽  
L. F. Cohen
Keyword(s):  
Thin Film ◽  
Magnetic Fields ◽  
Low Temperatures ◽  
Alternating Current ◽  
High Magnetic Fields

On the comparison of the platinum scale of temperature with the normal scale at temperatures between 444° and —190°C., with notes on constant temperatures below the melting-point of ice.

1905 ◽  
Vol 74 (497-506) ◽  
pp. 528-538 ◽  
Author(s):  
Morris William Travers ◽  
A. G. C. Gwyer
Keyword(s):  
Melting Point ◽  
Low Temperatures ◽  
Initial Pressure ◽  
Platinum Resistance Thermometer ◽  
Constant Volume ◽  
Platinum Resistance ◽  
Resistance Thermometer ◽  
Normal Scale

Introduction .—During the last few years one of us has been engaged in researches involving the accurate measurement of low temperatures. The measurements were made by means of gas thermometers, of the constant volume type, filled with hydrogen, or with helium, at an initial pressure of 1000 mm. As, however, this method proved cumbrous and inconvenient, it was decided to standardise a platinum resistance thermometer of the Callendar type against the gas thermometer, and to employ it in future investigations.

HYDROGEN PEROXIDE AND ITS ANALOGUES: II. PHASE EQUILIBRIUM IN THE SYSTEM HYDROGEN PEROXIDE – WATER

1951 ◽  
Vol 29 (2) ◽  
pp. 123-132 ◽  
Author(s):  
William T. Foley ◽  
Paul A. Giguère
Keyword(s):  
Hydrogen Peroxide ◽  
Phase Equilibrium ◽  
Solid Solutions ◽  
Freezing Point ◽  
Platinum Resistance Thermometer ◽  
Platinum Resistance ◽  
Radioactive Tracers ◽  
Resistance Thermometer ◽  
Pure Solution

A precision freezing point apparatus with platinum resistance thermometer was used to investigate the system hydrogen peroxide – water over the whole concentration range. The freezing point of the purest sample of hydrogen peroxide obtained by repeated fractional crystallizations of a large quantity of 99.6% pure solution was found to be −0.461°C; that of the dihydrate was −52.10°C. The two eutectics occur at concentrations of 45.2% and 61.2% H2O2 and at temperatures of −52.4° and −56.5°C. respectively. Contrary to what has been reported previously, water and hydrogen peroxide do not form solid solutions together. This was proved conclusively by applying the technique of radioactive tracers to the 'wet residue' method of Schreinemakers.

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