scholarly journals II. On the construction of some mercury standards of resistance, with a determination of the temperature coefficient of resistance of mercury

1905 ◽  
Vol 204 (372-386) ◽  
pp. 57-120 ◽  
Keyword(s):  
Electrical Measurement ◽  
National Physical Laboratory ◽  
Probable Error ◽  
Electrical Measurements ◽  
Temperature Coefficient Of Resistance ◽  
Cross Sectional ◽  
Object A ◽  
Physical Laboratory ◽  
Long Time

According to the Order in Council of August 23, 1894, by which certain fundamental electrical units were made legal— “The ohm which has the value 10 9 in terms of the centimetre, and the second of time, and is represented by the resistance offered to an unvarying electric current by a column of mercury at the temperature of melting ice, 14.4521 grammes in mass, of a constant cross-sectional area, and of a length 106.3 centims.,” is one of the units of electrical measurement on which “denomination of standards required for use in trade” is to be based. The establishment of the National Physical Laboratory rendered it possible to realize this unit in England. With this object, a number of selected tubes of “Verre dur” were obtained from M. Baudin, with the kind assistance of the officials of the Bureau International, while others of Jena 16'" glass were procured from Messrs. Schott and Co., Jena. The work, however, has necessarily occupied a long time. With the increasing accuracy of electrical measurements it appeared desirable to determine the constants of the tubes so that the probable error should not exceed 1 part in 100,000. Preliminary observations of various kinds were essential to secure success, while the work of organising the various departments of the Laboratory also tended to delay matters; hence it was not until the autumn of 1902 that the real start was made.

scholarly journals On the construction of some mercury standards of resistance, with a determination of the temperature coefficient of resistance of mercury.

1904 ◽  
Vol 73 (488-496) ◽  
pp. 239-243
Author(s):  
F. E. Smith ◽  
Richard Tetley Glazebrook
Keyword(s):  
Temperature Coefficient ◽  
National Physical Laboratory ◽  
Temperature Coefficient Of Resistance ◽  
Physical Laboratory

This paper contains an account of the construction and measurement of eleven mercury standards of resistance at the National Physical Laboratory, Teddington.

scholarly journals Gordon Brims Black McIvor Sutherland, 8 April 1907 - 27 June 1980

1982 ◽  
Vol 28 ◽  
pp. 589-626 ◽  
Keyword(s):  
Molecular Structure ◽  
Critical Time ◽  
Active Role ◽  
The United States ◽  
National Physical Laboratory ◽  
Andrews University ◽  
Left Behind ◽  
Active Life ◽  
Physical Laboratory

As a scientist Gordon Sutherland made, at a critical time, a major contribution to the transformation of infrared spectroscopy from a research technique practised in few laboratories into a powerful and widely used method for analysis and for the determination of molecular structure. A physicist by training, he was happy to be described as a chemical physicist or a biophysicist in relation to different aspects of his researches. Later in his career he was a successful Director of the National Physical Laboratory and then Master of Emmanuel College, Cambridge. He played an active role in British science policy. He died on 27 June 1980, in his seventy-third year, some 3 years after his retirement from the Mastership of Emmanuel College. Although after his graduation from St Andrews University Sutherland spent most of his active life in England or in the United States, he always retained the accent of a Scot, and a very deep affection for his native country. In a characteristically thoughtful way, Sutherland left behind a brief account in his own words of the earlier part of his life and career. A number of substantial quotations from his autobiographical document are included in this memoir.

scholarly journals The thermal and electrical conductivity of a single crystal of aluminium

1927 ◽  
Vol 115 (770) ◽  
pp. 236-241 ◽  
Keyword(s):  
Electrical Conductivity ◽  
Single Crystals ◽  
Test Specimen ◽  
Average Diameter ◽  
National Physical Laboratory ◽  
Present Communication ◽  
Uniform Size ◽  
The Third ◽  
Physical Laboratory

The recent work of Carpenter and Elam on the growth of single crystals of large dimensions has rendered possible the study of the physical constants of single crystals of the commoner metals, and the present communication describes the determination of the thermal and electrical conductivity of aluminium in the form of an isolated crystal. The form of the crystal investigated is shown in fig. 1. This crystal had been prepared at the National Physical Laboratory employing the technique described by Carpenter in “Nature,” p. 266, August 21, 1926, which briefly is as follows:— The test specimen is machined and subjected to three treatments, thermal, mechanical, and thermal. The first treatment is necessary to soften the metal completely and produce new equiaxed crystals of so far as possible uniform size, the average diameter being 1/150 inch. The second consists in straining these crystals to the required amount, and the third in heating the strained crystals to the requisite temperature, so that the potentiality of growth conferred by strain could be brought fully into operation.

Address of the President, Professor P. M. S. Blackett, C.H., at the Anniversary Meeting, 30 November 1966

1967 ◽  
Vol 167 (1006) ◽  
Keyword(s):  
National Physical Laboratory ◽  
Simple Approach ◽  
Ionic Crystals ◽  
X Ray Diffraction ◽  
Complete Structure ◽  
Principal Role ◽  
X Ray ◽  
Physical Laboratory ◽  
Royal Institution

The Copley Medal is awarded to Sir Lawrence Bragg, O.B.E., M.C., F.R.S. Bragg’s career has precisely coincided with the growth of a major field of science—the X-ray diffraction analysis of crystal structures. This had its beginning in his own early researches, and he has throughout played a principal role by his leadership at a series of laboratories, at Manchester, at the National Physical Laboratory, at Cambridge and at the Royal Institution, and in many other ways. He was the first to determine the atomic arrangement in a crystal (sodium chloride), and this work marked the introduction of a technique which has since been successfully applied to increasingly complicated molecules, culminating in the complete structure determination of the protein lysozyme at the Royal Institution a year before his retirement. Bragg has been prominent in the development of methods, beginning with the Law named after him; he also pioneered or encouraged the application of these methods in several fields—ionic crystals, elementary oxides, silicates, metals and proteins. The striking characteristic of Bragg as a scientist has been his direct and simple approach to complicated physical situations; his solutions of problems have a lucidity and simplicity which, in retrospect, make one forget how baffling they often seemed in advance.

scholarly journals On the determination of the absolute unit of resistance by alternating current methods

1912 ◽  
Vol 87 (597) ◽  
pp. 391-414 ◽  
Keyword(s):  
Lower Order ◽  
Alternating Current ◽  
National Physical Laboratory ◽  
Mutual Inductance ◽  
Electrical Circuits ◽  
Physical Laboratory ◽  
Absolute Measure ◽  
The Absolute ◽  
Set Up

1. Introductory .—Recently at the National Physical Laboratory we have constructed a standard of mutual inductance of novel type, whose value has been accurately calculated from the dimensions. This inductance has formed the basis for the determination of the unit of resistance in absolute measure by two different methods, in both of which alternating current is employed. Although there is no doubt that the accuracy attainable by these methods could be increased by greater elaboration of the apparatus used, the results already obtained seem to be of sufficient interest to warrant publication. It should be mentioned that the accuracy here aimed at was of a considerably lower order than that contemplated in the determination of the ohm by the Lorenz apparatus which is at present being carried out in the laboratory. For the experiments here described, no apparatus was specially constructed, but use was made of instruments which had already been designed and set up for the measurement of inductance and capacity. I shall first give a brief description of the standard inductance and then pass on to the methods and results. 2. Standard Mutual Inductance .—The design of the mutual inductance has already been described. The electrical circuits have the form and arrange­ment shown in section in fig. 1.

scholarly journals The optical determination of high metallurgical temperatures - The melting point of iron

1930 ◽  
Vol 129 (809) ◽  
pp. 91-114
Keyword(s):  
Melting Point ◽  
Molten Metal ◽  
National Physical Laboratory ◽  
Optical Pyrometer ◽  
Chemical Attack ◽  
Physical Laboratory ◽  
Thermal Changes ◽  
Refractory Crucible ◽  
Optical Determination

The present investigation has been carried out in the Metallurgical Department of the National Physical Laboratory in order to adapt the optical pyrometer to the estimation of the fusion temperatures of materials of high purity and high melting point and of substances of corrosive or volatile nature. Melting points and thermal changes in the solid state at high temperatures are generally determined by means of platinum thermocouples which are protected from the molten metal or its vapour by insertion in a refractory sheath. Contamination of the molten metal is frequently occasioned by chemical attack which takes place between the metal and the refractory crucible or couple sheath. This is particularly marked when the refractories contain siliceous material.

scholarly journals On a standard of mutual inductance

1907 ◽  
Vol 79 (532) ◽  
pp. 428-435 ◽  
Keyword(s):  
National Physical Laboratory ◽  
Mutual Inductance ◽  
Electrical Measurements ◽  
Working Standard ◽  
Standard Unit ◽  
Magnetic Testing ◽  
Physical Laboratory ◽  
Rayleigh Method ◽  
Geometrical Dimensions ◽  
Commutator Method

1. Introductory .—In many electrical measurements, such as those of capacity and inductance, as well as in the magnetic testing of iron, an accurately known standard of mutual inductance is of great value. It is sometimes convenient to derive such a standard from the standard unit of resistance, and this may be done in several ways, for example, by the well-known method of the ballistic galvanometer; or by Carey Foster’s method the mutual inductions may be tested against a condenser whose capacity has been found in terms of resistance and frequency by Maxwell’s commutator method; or it may be obtained directly in similar terms by the help of an unknown inductance by the Hughes-Rayleigh method. In the National Physical Laboratory I have used both of these latter methods (with the help of a vibration galvanometer) to obtain a working standard of mutual inductance. But this procedure is somewhat illogical, seeing that the unit of resistance has been itself commonly determined by the aid of mutual inductances calculated from the dimension of the coils or other conductors used; thus for the highest accuracy it is desirable to revert to a standard whose value can be determined solely from the geometrical dimensions. Accordingly, some eighteen months ago, I took in hand the investigation of a suitable design for such a standard, and I proceed to describe the result at which I arrived.

scholarly journals On the effect of the form of the transverse section on the frictional resistance to the motion of an elongated body parallel to its length through a fluid

1915 ◽  
Vol 92 (636) ◽  
pp. 144-157 ◽  
Keyword(s):  
Eddy Currents ◽  
Transverse Section ◽  
Practical Importance ◽  
Frictional Resistance ◽  
National Physical Laboratory ◽  
Cornell University ◽  
Physical Laboratory ◽  
Series Of Experiments ◽  
The Subject

1. The great increase in tire lengths of the parallel mid-bodies of recently constructed submarines and airships has raised into prominence the question of the frictional resistance of such elongated bodies moving parallel to their length through fluids, like air and water, whose viscosities cannot be neglected. This resistance increases as the length increases, and benefits comparable with the head and tail resistances, which for short bodies constitute nearly the whole resistance. In general, the problem of greatest practical importance is the determination of the frictional resistance when the motion is rapid enough to produce eddy currents in the fluid, but the difficulties in the way of a general theory of eddy current motion have presented a solution being reached. The simpler problem of the resistance offered by the walls of a circular pipe to the turbulent flow of viscous fluid through the pipe formed the subject of extensive series of experiments by Saph and Schoder, of Cornell University, and by Stanton and Pannell at the National Physical Laboratory.

AN IMPROVED INTERFEROMETER FOR DETERMINING PARALLELISM ERRORS IN LONG END-GAUGES

1947 ◽  
Vol 25f (3) ◽  
pp. 242-259
Author(s):  
L. Graham Turnbull
Keyword(s):  
Mechanical Design ◽  
National Physical Laboratory ◽  
Physical Laboratory ◽  
Specialized Technique ◽  
End Gauges ◽  
The Difference

This paper describes an interferometer designed for the determination of the parallelism of the working faces of end-gauges up to 24 in. in length. An instrument for this purpose, but which required somewhat highly specialized technique in the course of its construction, had been previously designed by the National Physical Laboratory. Using optical principles the same as those of the British instrument, another of an entirely new mechanical design has been constructed by the National Research Laboratories, Ottawa. This new interferometer incorporates kinematic principles and a number of interesting features to permit easy adjustment and operation to the very fine limits necessary. By the addition of a sensitive level vial to this instrument, the difference in length of nominally equal end-gauges can be determined to an accuracy of 1 or 2 × 10−6 in.

Sign in / Sign up

Export Citation Format

Share Document