The ITS-90 Temperature of the Gallium Melting Point and the Mercury Freezing Point

Metrologia ◽  
1995 ◽  
Vol 31 (5) ◽  
pp. 399-400 ◽  
Author(s):  
L Crovini
1977 ◽  
Vol 23 (4) ◽  
pp. 719-724 ◽  
Author(s):  
Donald D Thornton

Abstract The sharpness and reproducibility of the gallium melting point were studied, and the melting temperature of gallium in terms of IPTS-68 was determined. Small melting-point cells designed for use with thermistors are described. Nine gallium cells including three levels of purity were used in 68 separate determinations of the melting point. The melting point of 99.99999% pure gallium in terms of IPTS-68 is found to be 29.7714 ± 0.0014 °C; the melting range is less than 0.0005 °C and is reproducible to ±0.0004 °C.


1857 ◽  
Vol 8 ◽  
pp. 455-458 ◽  

The object of this communication is to lay before the Royal Society a theory which I have to propose for explaining the plasticity of ice at the freezing point, which is shown by observations by Professor James Forbes, and which is the principle of his Theory of Glaciers. This speculation occurred to me mainly in or about the year 1848. I was led to it from a previous theoretical deduction at which I had arrived, namely, that the freezing point of water, or the melting point of ice, must vary with the pressure to which the water or the ice is subjected, the temperature of freezing or melting being lowered as the pressure is increased.


1983 ◽  
Vol 61 (10) ◽  
pp. 1116-1121
Author(s):  
Jean-Pierre Caillé

The freezing point and the melting point of myoplasm were measured with two experimental models. In all samples, a supercooled stage was reached by lowering the temperature of the sample to approximately −7 °C, and the freezing of the sample was mechanically induced. The freezing process was associated with a phase transition in the interstices between the contractile filaments. In intact muscle fibers, the freezing point showed a structural component (0.43 °C), and the melting point indicated that the intracellular and the extracellular compartments are isotonic. When the sample of myoplasm, previously inserted in a cylindrical cavity was incubated in an electrolyte solution, the freezing point showed a structural component similar to that of the intact muscle fiber, but the melting point was lower than the freezing and the melting points of the embedding solution. This was interpreted as evidence that the counterions around the contractile filaments occupied a nonnegligible fraction of the intracellular compartment.


1972 ◽  
Vol 50 (6) ◽  
pp. 839-843 ◽  
Author(s):  
J. F. Maillot ◽  
D. R. Morris

The system calcium chloride – calcium carbide has been examined by thermal analysis. The depression of the freezing point of CaCl2 by CaC2 is ideal. The system is a eutectic one, with a eutectic point at 90 mol% CaCl2 at 740 °C. Carbon is believed to be present in the electrolyte as the so called acetylide ion [Formula: see text] The melting point of pure CaCl2 was found to be 775.2 ± 0.6 °C.


The object for which the present investigation was undertaken was to study the spontaneous crystallisation of mixtures of two substances which form mixed crystals and possess a minimum, or eutectic, freezing point. According to Cady, naphthalene and monochloracetic acid are such a pair of substances, and possess a minimum melting point of 53°·5 for the eutectic mixture of 29·4 per cent, naphthalene, 70·6 per cent, monochloracetic acid. We have attempted to verify Cady’s freezing and melting point curves, but, although our experiments confirm the former, we were quite unable to verify the latter. Pickering mentions four modifications of monochloracetic acid, and traces the freezing point curves for three of them. Our study of mixtures of monochloracetic acid and naphthalene has not given us the information we expected concerning the composition of the “mixed crystals” which separate spontaneously from a solution, but it has led to interesting results concerning the spontaneous crystallisation of the different modifications of a substance dissolved in another substance which is not polymorphous. The Different Modifications of Monochloracetic Acid and their Mutual Transformations . Microscopic examination of crystals of monochloracetic acid obtained from fusion or solution show clearly that three different modifications α, β , and γ of the acid exist. These modifications have melting points 61˚˙5, 55°, and 50°; they are formed on the microscope slide under different circumstances, each modification yielding rhombs quite distinct from those of the two other modifications. If fused monochloracetic acid be cooled suddenly it crystallises as the γ -modification in rhombs having a plane angle of about 59°. If these rhombs be touched they at once transform into the β -modification and give rhombs having a plane angle of about 72°; or occasionally the γ -rhombs are transformed at once into the stable a-modification of the acid, which exists as broad needles having an acute angle of 43˚. The transformation from γ to α takes place much more rapidly than the transformation from γ to β . Similarly, if rhombs of β are formed on a microscope slide they may be at once transformed into the α -modification by inoculating with a fragment of α . Each transformation is accompanied by a rise of temperature. A remarkable feature of the change is that the more stable modification crystallises with sharp edges in the solid mass of the less stable substance, as though it were growing in a liquid.


Molecules ◽  
2020 ◽  
Vol 25 (18) ◽  
pp. 4290 ◽  
Author(s):  
Daniel Lozano-Martín ◽  
Salomé Inês Cardoso Vieira ◽  
Xavier Paredes ◽  
Maria José Vitoriano Lourenço ◽  
Carlos A. Nieto de Castro ◽  
...  

Ionic liquids have been suggested as new engineering fluids, namely in the area of heat transfer, as alternatives to current biphenyl and diphenyl oxide, alkylated aromatics and dimethyl polysiloxane oils, which degrade above 200 °C and pose some environmental problems. Recently, we have proposed 1-ethyl-3-methylimidazolium methanesulfonate, [C2mim][CH3SO3], as a new heat transfer fluid, because of its thermophysical and toxicological properties. However, there are some interesting points raised in this work, namely the possibility of the existence of liquid metastability below the melting point (303 K) or second order-disorder transitions (λ-type) before reaching the calorimetric freezing point. This paper analyses in more detail this zone of the phase diagram of the pure fluid, by reporting accurate thermal-conductivity measurements between 278 and 355 K with an estimated uncertainty of 2% at a 95% confidence level. A new value of the melting temperature is also reported, Tmelt = 307.8 ± 1 K. Results obtained support liquid metastability behaviour in the solid-phase region and permit the use of this ionic liquid at a heat transfer fluid at temperatures below its melting point. Thermal conductivity models based on Bridgman theory and estimation formulas were also used in this work, failing to predict the experimental data within its uncertainty.


1977 ◽  
Vol 23 (4) ◽  
pp. 711-718 ◽  
Author(s):  
B W Mangum

Abstract The latest internationally-adopted temperature scale, the International Practical Temperature Scale of 1968 (amended edition of 1975), is discussed in some detail and a brief description is given of its evolution. The melting point of high-purity gallium (stated to be at least 99.99999 % pure) as a secondary temperature reference point is evaluated. I believe that this melting-point tem-perature of gallium should be adopted by the various medical professional societies and voluntary standards groups as the reaction temperature for enzyme reference methods in clinical enzymology. Gallium melting-point cells are available at the National Bureau of Standards as Standard Reference Material No. 1968.


The death of Mr. C. T. Heycook, which took place oil June 3, removes from among us one who has gained the affection of generations of Cambridge men and who was a pioneer in an important branch of inorganic chemistry. Heycock was the younger son of Frederick Heycock, of Braunston, Oakham, and was born on August 21, 1858; he received his early education at the Grammar Schools of Bedford and Oakham, and entered King's College, Cam-bridge, as an Exhibitioner in 1877, taking the Natural Sciences Tripos in 1880. For many years he taught Chemistry, Physics and Mineralogy for the Cambridge examinations and in 1895 he was elected to a Fellowship at King’s College, becoming a College lecturer and Natural Sciences Tutor in the following year, lie was elected a Fellow of the Royal Society in 1895 and was awarded the Davy Medal in 1920 for his work on alloys. His original work on the metals attracted the attention of the Goldsmiths Company who endowed a Readership in Metallurgy at Cambridge; he was appointed to this office in 1908 and held it until his retirement in 1928. He was admitted to the Livery of the Gold-smiths Company in 1909 and to the Court in 1913; he acted as Prime Warden during the year 1922-1923 and took a been interest in the work of the Company’s Assay Office. Notwithstanding the exacting character of his work as a Cambridge coach, Heycock joined with his lifelong friend, F. H. Neville, F.R.S., in a comprehensive study of the metals and their alloys; this partnership, which was only dissolved by the death of Neville in 1915, led to a remarkable series of papers in which novel directions of investigation were mapped out and developed. Before entering upon this joint work, Heycock had had some experience as an investigator; in 1876 he published a not on the spectrum of indium in conjunction with Mr. A. W. Clayden, M. A., and in 1882 he contributed a paper on the atomic weight of rubidium at the British Association meeting. Heycock and Neville’s first joint paper was published in 1884 and described a redetermination of the molecular weight of ozone by the diffusion method. The first of the series of papers on the metals was published in 1889 and dealt with the depression of the freezing points of metals brought about by others dissolved therein; in this, and later papers, it was shown that the addition of small amounts of a second metal depresses the freezing point of the first to an extent (1) directly proportionate to the weight, of metal added, and (2) in rough inverse proportion to the atomic or molecular weight of the added metal. Raoult’s law for ordinary solutions was thus extended to alloys and a method indicated for calculating the latent heat of fusion of a metal by the application to the freezing point depressions of the now well-known van't Hoff equation. At the outset mercury thermometers were used in the temperature measurements and only alloys of low melting points could be studied: the introduction by H. L. Callendar of the platinum resistance pyrometer made it possible to extend the scope of the investigation to metals of high melting point. At that time the melting points of silver, gold and copper were not known with any degree of accuracy, partly because of the difficulty of making the physical measurements, partly because the necessity for using metals of high chemical purity and for protecting them from contamination during melting had not been recognised. A number of fixed points on the platinum resistance pyrometer had to be established before the study of alloys of high melting points was undertaken; these fixed points were determined with the aid of Dr. E. H. Griffiths, F. R. S., and with such accuracy that the results obtained by their use have not since been seriously affected. Thus, Heycock and Neville determined the melting point of Levol’s alloy as 778.7° C. and used this constant as a secondary fixed point; a very recent determination by the Washington Bureau of Standards gives the melting point as 779.4°.


1954 ◽  
Vol 32 (5) ◽  
pp. 550-556 ◽  
Author(s):  
Paul A. Giguère ◽  
E. A. Secco

The cooling curves of a number of solutions of deuterium peroxide in heavy water in the concentration range 11% to 95% were measured in order to determine the solid-liquid phase diagram for that binary system. The apparatus of Herington and Handley, which uses a pulsing pressure for stirring the solutions, and a thermistor, was found to be particularly suitable for that purpose. As could be expected the freezing-point curve of the deuterated compounds is closely similar to that of the hydrogen compounds, being shifted up only by about 4° for water-rich solutions and by 2° for peroxide-rich solutions. The melting point of the addition compound, D2O.2D2O very nearly coincides with one of the eutectic points at 46.2% D2O2 and −51.5 °C.; the other eutectic point is at 60.5% D2O2 and −55.1 °C. By extrapolation the melting point of pure deuterium peroxide is found to be 1.5 °C. as compared with −0.43 °C. for hydrogen peroxide. Concentrated solutions of deuterium peroxide exhibit an extreme tendency to supercool, resulting sometimes in formation of glasses even at liquid-air temperature. The previous results of Foley and Giguère for the system H2O–H2O2 were confirmed, specially as regards the melting point of the addition compound H2O2•2H2O.


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