scholarly journals The effect of hydrogen on the discharge of negative electricity from hot platinum

The effect of hydrogen on the discharge of negative electricity from hot platinum was examined by the writer in 1903; it was found to produce a very large increase in the current. The experiments were all done with nearly new platinum wires which had not been heated in the gas for any great length of time, because it was known that long-continued heating causes the wire to disintegrate. The present paper contains an account of a series of experiments in which wires were heated for long periods in hydrogen, so that any changes in the effect of the hydrogen could be observed. It appears that continued heating in hydrogen alters the character of the effects observed so that the behaviour of an old wire may be very different from that of a new one. The following gives a short abstract of each section of the paper:— 1. Assuming that x = B p n , where x denotes the current per square centimetre of platinum at constant temperature, p is the pressure of the hydrogen, and B and n are quantities depending only on the temperature, and also that x = A θ ½ e –Q/2θ , where θ denotes the absolute temperature and A and Q depend only on the pressure; it is proved that: (1) n xθ -1– c , where α and c are constants; (2) Q = P — 2 α log p ; and (3) A = K p -c . These equations are shown to agree with the observations.

The effect of hydrogen on the discharge of negative electricity from hot platinum was examined by the writer in 1903 (‘Phil. Trans.,’ A, 352, vol. 202, 1903); it was found to produce a very large increase in the current carried by the discharge. At pressures below 0·1 millim. of mercury the leak was found to increase with the pressure and to fall when the pressure was reduced. The experiments in the paper just referred to were all done with nearly new platinum wires which had not been heated in the gas for any great length of time, because it was known that long continued heating caused the wire to disintegrate, its surface becoming covered with a network of cracks. The present paper contains an account of a series of experiments in which wires were heated for long periods in hydrogen, so that any gradual changes in the effect of the hydrogen could be observed. It appears that continued heating in hydrogen alters the character of the effects observed, so that the behaviour of an old wire may be very different from that of a new one. In the previous paper I suggested that the effect of hydrogen was due to the presence of hydrogen in the surface layer of the platinum, and this view appeared to be supported by the facts. Professor O. W. Richardson (‘Phil. Trans.,’ A, 413, vol. 207, 1906) puts forward a different theory, viz., that the hydrogen alters the state of the platinum, so that the effect may remain even after the removal of all the hydrogen.


The relation between the thermal and electrical conductivities of me has for a long time engaged the attention of physicists. As far back as 1 Wiedemann and Franz propounded the law to the effect that the ratio of two conductivities was the same for all metals. In 1872 Lorenz, both on retical and experimental grounds, sought to establish that the above-mentio ratio was proportional to the absolute temperature. On the development the electron theory Drude, H. A. Lorentz, J. J. Thomson and others ha on the basis of various assumptions, arrived at the same conclusion as Lon Up to 1900, however, the experimental values were too uncertain to allow definite confirmation of the theory. In that year Jaeger and Diesselho published the result of their investigation, which gave directly the ratio of conductivities for a number of metals and alloys over the range 18° to 100° Lees has since, by an independent method, confirmed the values of Jaeger Diesselhorst for a number of metals at 18° C. and has carried the investigat own to —170° C. Meissner has experimented with some pure metals down —250° C. and Onnes and Holst even lower. The result of these investigations has been to show that between —100° C. + 100° C. the value of the function K/ λ T (K and λ being the thermal and ectrical conductivities and T the absolute temperature), is sensibly the samer the pure metals, with perhaps a slight tendency to fall with decreasing temrature. Below —100° C., however, the function shows an increasingly rapid with temperature and a considerable divergence between individual metals, ove a temperature of + 100° C. very few determinations of thermal conictivity have been made, and the object of the present series of experiments is been to measure, in this region, the thermal and electrical conductivities a number of metals of the highest purity obtainable commercially.


The specific heats of three paramagnetic salts, neodymium magnesium nitrate, manganous ammonium sulphate and ferric ammonium alum, have been measured at temperatures below 1°K using the method of γ -ray heating. The temperature measurements were made in the first instance in terms of the magnetic susceptibilities of the salts, the relation of the susceptibility to the absolute temperature having been determined for each salt in earlier experiments. The γ -ray heatings gave the specific heat in arbitrary units. The absolute values of the specific heats were found by extrapolating the results of paramagnetic relaxation measurements at higher temperatures. The measured specific heat of neodymium magnesium nitrate is compared with the value calculated from paramagnetic resonance data, and good agreement is found.


1899 ◽  
Vol 22 ◽  
pp. 598-600
Author(s):  
Dr W. Peddie

In 1865 Lord Kelvin published the results of experiments which first made evident “a very remarkable fatigue of elasticity, according to which a wire which has been kept vibrating for several hours or days through a certain range came to rest much quicker when left to itself than when set in vibration after it has been at rest for several days and then immediately left to itself.” On the strength of Lord Kelvin's statement this elastic fatigue of metals has been regarded as a definitely ascertained fact. But, quite recently (Physical Review, March 1899), Mr Joseph O. Thompson has published a paper “On the period and logarithmic decrement of a continuously vibrating wire,” in which he states that it seems probable that “for constant temperature and constant amplitude the logarithmic decrement is constant.” This conclusion is based upon his observation that the logarithmic decrement, in the case of a copper wire, when the amplitude of vibration varied from about 185° to 175°, had the same value after it had been continuously vibrated through the average arc of 180° for fifty consecutive hours as it had at the commencement of that period. Observations upon other metals seemed to support the conclusion.Lord Kelvin also stated that fatigue caused an increase of the period of vibration. Mr Thompson finds that “no matter what metal was used, no matter whether the arc of vibration was as small as 20° or as high as 200°, no matter whether the wire was long or short, thick or thin (provided of course the breaking strength of the wire was at least twice the weight of the disc), the result was uniformly the same, namely, that when temperature and amplitude of vibration remained constant, the period of vibration was a constant quantity.”


1973 ◽  
Vol 95 (2) ◽  
pp. 236-241
Author(s):  
T. F. Ford ◽  
C. R. Singleterry

Many relationships between viscosity or its reciprocal, fluidity, and temperature have been proposed for liquids. None except the empirically modified ASTM chart have proven satisfactory over extended temperature ranges. We here note that by plotting the kinematic fluidity (φkin) against the square of the absolute temperature (deg K2) we obtain linear relationships for a wide variety of organic liquids at kinematic viscosities less than about 1.67 centistokes (or fluidities above about 0.60 reciprocal centistokes). The generality of the relationship appears to justify the use of the equation, φkin=a+bT2, as an interpolation formula for organic liquids in the low viscosity region.


2021 ◽  
Vol 33 (2) ◽  
pp. 9-19
Author(s):  
V. VIJAYAKUMAR ◽  

The measured thermal radiation from a material surface will, in general, have a wave length (\lambda) dependent scale-factor to the Planck profile (PT) from the contributions of the emissivity (Є\lambda) of the surface, the response function (A\lambda) of the measurement setup, and the emission via non-Plank processes. For obtaining the absolute temperature from such a profile, a procedure that take care of these dependencies and which relay on a temperature grid searchis proposed. In the procedure, the deviation between the Plank profiles at various temperatures and the measured spectrum that is made equal to it at a selected wavelength, by scaling, is used. The response function (A\lambda) is eliminated at the measurement stage and the polynomial dependence of the remnant scale factor mostly dominated by Є\lambda) i s extracted from the measured spectrum by identifying its optimal \lambda dependence. It is shown that when such a computation is carried out over a temperature grid, the absolute temperature can be identified from the minimum of the above deviation. Here, search for T and Є\lambda) d elinked, unlike in the leastsquare approaches that are normally employed. Code that implements the procedure is tested with simulated Planck profile to which different viable values of Є\lambda) a nd noise is incorporated. It shown that if the \lambda dependence of scale-factor is not too high, the absolute temperature can be recovered. A large \lambda dependent scale-factor and the consequent possible error in the temperature obtained can also be identified.


2003 ◽  
Vol 83 (1) ◽  
pp. 15-30 ◽  
Author(s):  
Goran Andjelkovic

The urban heat island, as a phenomenon due to the higher air temperature in the cities as compared to their immediate surroundings, represents the most important consequence of the urbanization influence on the topoclimate. As compared to the smaller cities in its surroundings, Belgrade's average annual temperature is from 0,4 to 1,0 ?C higher (period 1961-1990). A very liable index of the Belgrade's heat island is the air temperature measured at the airport in Surcin. In the period from 1971-1990. average annual air temperature at the airport was 11,2 ?C, and in the city center it was 0,7 ?C higher. Belgrade has a higher absolute minimal temperature than its surroundings during every month. In the last climatic period the absolute temperature minimum in Belgrade was even 5,4 ?C higher than the highest value measured within this parameter in its wider surroundings (Veliko Gradiste -26,4 ?C). In the above mentioned twenty years period the absolute air temperature minimum in Surcin was -26,0 ?C, and in the city center only -18,2 ?C. The number of the frosty days at the airport was 77,8, and in Belgrade 58,2. Although the heat island of Belgrade was formed together with formation of the city, it was more evident at the beginning of the 20th century (0,4 ?C). During the next five to six decades a faster intensity growth was recorded (up to 0,9 ?C). This coincides with the period of the population growth as well as with development of the city activities, industry above all. During one year the intensity of the Belgrade's heat island reached its maximum in winter. In January the city, as compared to Surcin, was warmer for about 1,0 ?C, and in September for only 0,1 ?C. The daily variations of the heat island are such that it reaches its highest intensity during the evening hours (at 9 p.m. 0,9 ?C). If the average values of the extreme daily temperatures are being examined, one can see a distinct difference: average city minimums are 1,5 ?C higher than the airport minimums, while the maximums are only 0,2 ?C higher. During winter, in concrete anticyclonic conditions, it can be 10 ?C warmer in the city than in the immediate surroundings. Together with the perennial growth of heat island intensity, its "space range" also expands. The space structure of the heat island is very distinct. Exceptions in the temperature values between certain points of measurements in the winter morning hours can go up to 6-8 ?C.


1953 ◽  
Vol 2 (1) ◽  
pp. 49-68 ◽  
Author(s):  
Otto Mangold ◽  
Italo Testa

SummaryTwins deriving from a single zygote were produced in Triton alpestris and Triton taeniatus by two different series of experiments. The first type of experiments proceeded, by means of a glass thread put on and cutting through the median plane of early gastrulae, to a division of these into two lateral (right and left) halves. These halves may give rise to normally formed identical twins (fig. 2), or to twins with more or less accentuated deficiencies on their inner sides (figg. 3 and 4). In extreme cases they may even produce left or right half-embryos, or much reduced malformations with very imperfect organ formation. Generally considered, the regolation in the head region is better than that in the tail one, and much better than in the trunk. Most of the heads show two eyes of equal size and normal position; in rare cases we encounter two eyes of different size, or synophthalmus or cyclopia. The «real» half-embryos have only one laterally situated eye (tab. 2). The normally formed identical twins deriving from half an egg each, develop into properly proportionned embryos of half the normal size; the resulting larvae reach the normal size of the equally-aged control larvae deriving from entire eggs, often before the stage of nourishment, (fig. 5, tab. 3).In the second series of experiments, an early gastrula was cut through in correspondence to the median plane, and then the complete presumptive epidermis of another gastrula and, respectively, of a third one, was stuck on to the wound surfaces of the halves in normal orientation (fig. 6). The right and the left combinations resulting therefrom give rise, in the original median line, to long, narrow and apparently somewhat too great neural plates, the external half-portion of which was fournished by the host half-gastrula and is somewhat more strongly developped than the inner half-portion deriving from the presumptive epidermis (fig. 7 a, b). This epidermis that was stuck on to the gastrula-halves' surfaces, takes part in the formation of the embryos either totally or at least for its greatest part. No perfect larvae will be formed (tab. 4). The head is always bilaterally developped, but it is often asymmetric and shows synophthalmous or cyclopic character (figg. 8, 9, 10, tab. 5). The trunk is sometimes normal (fig. 8 a), but it may also show an axial system of too great length (fig. 8 b), or dorsal deficiencies—often in the form of either symmetrical or asymmetrical Spina bifida—with dorsal incurvation (fig. 9 a, b). The tail can be either normal, or crooked, or defective, or doubled. In the best cases we see, in the first series of experiments, the regolation of the half-organiser of the gastrula-half into an entire organiser of half the normal size, while, in the second series of experiments, the regolation can produce an approximately normally sized entire organiser, which however, in the anterior head region is lacking of its full indutcive capacity.In both series of experiments the right hand member of the twins was observed to show inversion of the situs viscerum.


1992 ◽  
Vol 9 ◽  
pp. 297-298
Author(s):  
G. Sironi ◽  
G. Bonelli ◽  
M. Gervasi

AbstractWe are carrying on measurements of the absolute temperature of the CBR at various frequencies near and below 1 GHz, looking for so far undetected deviations from a planckian spectrum. The amplitude and frequency of those distortions can give precious information about the history of the Universe.


1864 ◽  
Vol 13 ◽  
pp. 204-217

The experiments upon which I have been engaged for some time past, in connexion with the manufacture and properties of gun-cotton, have brought under my notice some interesting points in the behaviour of both gun. cotton and gunpowder, when exposed to high temperatures, under parti­cular conditions. I believe that these phenomena have not been previously observed, at any rate to their full extent, and I therefore venture to lay before the Royal Society a brief account of them. Being anxious to possess some rapid method of testing the uniformity of products obtained by carrying out General von Lenk’s system of manu­facture of gun-cotton, I instituted experiments for the purpose of ascer­taining whether, by igniting equal weights of gun-cotton of the same com­position, by voltaic agency, within a partially exhausted vessel connected with a barometric tube, I could rely upon obtaining a uniform depression of the mercurial column, in different experiments made in atmospheres of uniform rarefaction, and whether slight differences in the composition of the gun-cotton would be indicated, with sufficient accuracy, by a corre­sponding difference in the volume of gas disengaged, or in the depression of the mercury. I found that, provided the mechanical condition of the gun-cotton, and its position with reference to the source of heat, were in all instances the same, the indications furnished by these experiments were sufficiently accurate for practical purposes. Each experiment was made with fifteen grains of gun-cotton, which were wrapped compactly round the platinum wire; the apparatus was exhausted until the column of mercury was raised to a height varying from 29 inches to 29·5 inches. The flash which accompanied the deflagration of the gun-cotton was apparently similar to that observed upon its ignition in open air ; but it was noticed that an interval of time always occurred between the first application of heat (or incandescence of the wire) and the flashing of the gun-cotton, and that during this interval there was a very perceptible fall of the column of mercury. On several occasions, when the gun-cotton, in the form of “roving,” or loosely twisted strand, was only laid over the wire, so that it hung down on either side, the red-hot wire simply cut it into two pieces, which fell to the bottom of the exhausted vessel, without continuing to burn. As these results appeared to indicate that the effects of heat upon gun-cotton, in a highly rarefied atmosphere, differed importantly from those observed under ordinary circumstances, or in a very imperfect va­cuum, a series of experiments, under variously modified conditions, was instituted, of which the following are the most important.


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