Physicists and Physicians Stories from the History of Medical Physics and Bioengineering

Total Page:16

File Type:pdf, Size:1020Kb

Physicists and Physicians Stories from the History of Medical Physics and Bioengineering Physicists and Physicians Stories from the history of medical physics and bioengineering HPA Lecture 20th ICMP, Brighton September 1 2013 Francis Duck University of Bath, UK [email protected] Four stories of medical physics Giovanni Borelli (1608-1679) Italian astrophysicist Bryan Robinson (1680-1754) Irish physician Jules Gavarret (1809-1890) French medical physicist Edith Stoney (1869-1938) British medical physicist Thomas Young Neil Arnott Herman von Helmholtz Ferdinand Monoyer Adolf Fick Carlos Matteucci Emil du Bois- Reymond Golding Bird John Draper Published 2013: 306 pages ISBN 978 1 903613 55 9 Institute of Physics and Engineering in Medicine, Fairmount House 230 Tadcaster Road, York, YO24 1ES, UK Giovanni Pisa Borelli (1608-79) “I undertook this work … to enlist Anatomy into Physics” “If the spine of a stevedore is bent and supports a load of 120 pounds carried on the neck, the force exerted by Nature in the intervertebral disks and in the extensor muscles of the spine is equal to 25585 pounds. The force exerted by the muscles alone is not less than 6404 pounds”. Is the heart on fire? • “To determine the temperature of the heart accurately, at Pisa, I took care of opening the chest of a live stag and immediately let a thermometer be introduced through the wound into the left ventricle of the heart. • I saw that the highest temperature of the heart did not exceed 40° (gradus 40) which is the usual temperature in the sun in the summer in our country. • Afterwards, using similar thermometers, I measured the temperature of the liver, lungs and intestines in the same stag alive. • It appeared that the heart has the same temperature as the other viscera” Publication of De Moto Animalium • De Moto Animalium was published in Rome in 2 volumes, in 1680 and 1681, just after Borelli’s death • Queen Christina of Sweden gave financial support “her generosity provided the poor Author with considerable funds to improve his destiny and for his work.” • Borelli’s scientific philosophy: he quotes Plato’s reply to the question “What does God do?” : “God exerts geometry”. Not all physicians agreed that iatrophysics was helpful “The Greatest Numbers of Professors of Medicine are declared Enemies to it , and make nothing of breaking their Jests upon Angles, Cylinders, Cones, Celerity, Percussion, Resistance and such like terms, which they say have no more to do with Physic, or the Human Body, than a Carpenter has to do in making Venice Treacle, or curing a fever” John Quincy, Medical Statica: Being the Aphorisms of Sanctorius Translated into English, 5th edition. London. 1737. Bryan Robinson (1680-1754) An Irish Newtonian Physician Robinson’s repetition of Santorius’ “insensible perspiration” experiment Studies on the properties of fibres •A human hair from a “a healthful young Woman 22 years of age” •The extension was measured after it had been held under tension for 2 minutes •Then it was “gently rub’d the Hair from End to End with a Feather dipp’d in some Fluid, and continued thus wetting it for one Minute” •Then the same tension for a further 2 minutes. •He tested the effects of 65 different liquids. “Sir Isaac Newton discovered the Causes of Muscular Motion, and Secretion; and likewise furnished materials for explaining Digestion, Nutrition and Respiration.” Bryan Robinson. A Treatise on the Animal Oeconomy. 1732. Dublin. Robinson’s “Newtonian” explanations Of muscular action: “begun in the nerves at their origin, has been proved to be the vibration of a very elastic fluid ……. by the Power of the Will, a vibrating Motion is excited in the Æther in those Ends of the Nerves which terminate in the Brain, that Motion is in a Instant propagated thro’ their solid and uniform Capillamenta to the Membranes of the Muscles, and excites a like Motion in the Æther lodged within those Membranes” Of secretion: “Sir Isaac Newton has proved from experiments that Particles of Light attract ardent spirits and oil more strongly than water”. Did Robinson misrepresent Newton’s views? • Newton’s Optiks Query 23: “Is not vision perform’d chiefly by the vibrations of this medium (the aether), excited in the bottom of the eye by the rays of light, and propagated through the … optick nerves into the place of sensation? • Newton’s Optiks Query 24 “Is not animal motion perform’d by the vibrations of this medium, excited in the brain by the power of the will, and propagated from thence through the … nerves into the muscles?” • Newton’s Optiks Query 30 “Are not gross bodies and light convertible into one another, and may not bodies receive much of their activity from the particles of light which enter their composition?” A definition of medical physics, 1814 Jean Hallé Professor of Medical Physics and Hygiene, Faculty of Medicine in Paris (1795-1822) Physics applied to • knowledge of the human body …, • to its conservation … • and to the cure of its illnesses. Jules Gavarret (1809-1890) The third Professor of Medical Physics at the Faculty of Medicine, Paris Jules Gavarret France 1809 Born at Astaffort, Lot-et-Garonne 1815 Battle of Waterloo 1824 King Charles X 1829-31 École polytechnique, Paris 1830 Revolution: King Louis-Philippe 1831-33 Military training 1833-40 Medical training in Paris 1840-44 Haematology research with Gabriel Andral 1844 Appointed as professor of medical physics 1847 Cross of the legion d’honneur 1848 Revolution ends monarchy nd 1860 Married Eudoxie Binesse 1852 Napoleon III: 2 Empire 1862 Officer of the legion d’honneur 1871 Siege of Paris 1872 3rd Republic 1885 Retired: made honorary professor 1885 Commander of the legion d’honneur 1890 Died Principes generaux de statistique medicale (1840) • Gavarret had attended a heated discussion on C-A Louis’ data on blood-letting with 140 typhoid patients. • “Navier’s discourse made clear his grasp of the subject and the judgements one could draw from the use of the principles of probability calculation in therapeutic research” • Gavarret applied Poisson’s probability calculations to Louis’ data. With a probability of just over 99.9 to 1, the true mortality rate could have been as high as 49% or as low as 26%. Charles- Claude- Alexandre Louis Siméon Louis Navier Poisson Becquerel’s thermocouple measurements Back’s Arctic measurements Regnault’s apparatus Books by Gavarret • 1840 Principes generaux de statistique medicale • 1855 De la chaleur produite par les êtres vivants • 1859 Traite de l’électricité • 1861 Télégraphique électriquea • 1866 Des images par réflexion et par réfraction • 1869 Physique biologique - Phénomènes physiques de la vie • 1877 Acoustique biologique – Phénomènes physiques de la phonation et de l’audition Is this wide and beautiful theory of reciprocity of forces general enough to encompass the dynamic appearances of the organized world as well as those of the inorganic world? Must it, in a word, be accepted to be universal? These are ideas on which we place reliance, so as to push back, as a mere useless hypothesis, the existence of that independent directing force exerted on the body which, under various names, the vitalist school invoke to explain the phenomena of nutrition and development. Gavarret and medical education • 1872 Strasbourg medical school closed and moved to Nancy • 1873 Gavarret appointed as inspector of preparatory medical schools to review upgrade to full faculty status. • 1874 Preparatory schools at Lyons and Bordeaux converted to full Faculties. • 1879 Gavarret appointed as Inspector-General for Higher Medical Education Professors of medical physics in French Medical Faculties Monoyer, Ferdinand (1836-1912) Lyon Imbert, Armand (1850-1922): Montpellier Charpentier, Augustin (1852-1916) Nancy Bergonié, Jean-Alban (1857-1925) Bordeaux Number of general medical physics books published per decade 6 5 4 3 France 2 Other countries 1 0 Biological physics syllabus • fluid mechanics and the circulation • pneumatics and respiration • optics and vision • acoustics and speech and hearing • heat and body temperature • dynamics and animal mechanics • electricity and bio-electrics • energy and metabolism He was by nature a true scientist, and I always knew him as a freethinker. And, if … his funeral honours did not conform in this regard to his ideas …. he might blame, no doubt, that impersonal posthumous tendency that is so easily assumed, without conscious thought or interest, under the cover and apparent benefit of outmoded, although sacred, customs. Voltaire himself did not escape M Laborde 1890 Edith Stoney MA (1869-1938) Edith Stoney’s family Cousin Father Distant cousin George FitzGerald FRS George Johnstone Stoney FRS Alan Turing (physicist) (physicist) (mathematician) Brother Brother Edith Sister Sister Gerald Stoney FRS Robert Stoney Stoney Florence Stoney Gertrude Stoney (engineer) (doctor) OBE (radiologist) (artist) Edith Stoney’s life • Born 6 January 1869: Donnybrook, Dublin. • 1890-94: Newnham College Cambridge. First class in Maths Tripos Part 1. • 1895-98: Mathematics teacher, Cheltenham Ladies College • 1899-1915 Lecturer in Physics, London (Royal Free) School of Medicine for Women • 1915-1919 Medical military service during WWI • 1919-1925 Lecturer in Physics, Household and Social Science Department, King’s College for Women. • 1925-1938. Retirement work with the British Federation of University Women • Died 25 June 1938: Bournemouth Edith Stoney as a mathematical physicist “The problems she has attacked and solved have been in relation to the special curvature of mirrors for obtaining beams of light of particular shapes. These investigations involved
Recommended publications
  • History of Physics Group Newsletter No 21 January 2007
    History of Physics Group Newsletter No 21 January 2007 Cover picture: Ludwig Boltzmann’s ‘Bicykel’ – a piece of apparatus designed by Boltzmann to demonstrate the effect of one electric circuit on another. This, and the picture of Boltzmann on page 27, are both reproduced by kind permission of Dr Wolfgang Kerber of the Österreichische Zentralbibliothek für Physik, Vienna. Contents Editorial 2 Group meetings AGM Report 3 AGM Lecture programme: ‘Life with Bragg’ by John Nye 6 ‘George Francis Fitzgerald (1851-1901) - Scientific Saint?’ by Denis Weaire 9 ‘Benjamin Franklin (1706-1790) - a brief biography by Peter Ford 15 Reports Oxford visit 24 EPS History of physics group meeting, Graz, Austria 27 European Society for the History of Science - 2nd International conference 30 Sir Joseph Rotblat conference, Liverpool 35 Features: ‘Did Einstein visit Bratislava or not?’ by Juraj Sebesta 39 ‘Wadham College, Oxford and the Experimental Tradition’ by Allan Chapman 44 Book reviews JD Bernal – The Sage of Science 54 Harwell – The Enigma Revealed 59 Web report 62 News 64 Next Group meeting 65 Committee and contacts 68 2 Editorial Browsing through a copy of the group’s ‘aims and objectives’, I notice that part of its aims are ‘to secure the written, oral and instrumental record of British physics and to foster a greater awareness concerning the history of physics among physicists’ and I think that over the years much has been achieved by the group in tackling this not inconsiderable challenge. One must remember, however, that the situation at the time this was written was very different from now.
    [Show full text]
  • Third ICESHS, Austrian Academy of Sciences, Vienna 2008 Electron – A
    Third ICESHS, Austrian Academy of Sciences, Vienna 2008 Isabel Serra, Francisca Viegas, Elisa Maia Department of History and Philosophy of Science, University of Lisbon Lisboa, Portugal [email protected] Electron – a main actor in scientific controversies1 1. Introduction The story of the electron can contribute to the study of the continuity-discontinuity of the scientific thinking in modern age, as well as to discuss models and metaphors in history of science. Actually, the electron played a central role in several scientific controversies: nature of electricity and cathode rays, structure and properties of matter. The idea of an atom of electricity was introduced by Faraday and adopted by Helmholtz. In 1874, Stoney estimated its charge and named it electron. However, Maxwell had stated that a complete knowledge of electricity would eliminate the necessity of such particles. The controversy about the nature of electricity was to lie dormant for years until it was brightened by the study of discharges in gases. The nature of cathode rays divided physicists and chemists, with the electron playing the major role in the dispute. The experiences of Perrin (1895) and Thomson (1897), seemed to confirm the existence of the electron, but did not convince all scientists. The electron became the main protagonist of a controversial image of matter: the atomistic view. In 1913, Bohr’s atomic theory was received with enthusiasm by some physicists but with criticism by others. Nevertheless, the atomic structure of matter gradually wins acceptance in reason of its extraordinary power in predicting spectral lines. At last, electrons were particles, coherent with facts and theories.
    [Show full text]
  • Should Physical Laws Be Unit-Invariant?
    Should physical laws be unit-invariant? 1. Introduction In a paper published in this journal in 2015, Sally Riordan reviews a recent debate about whether fundamental constants are really “constant”, or whether they may change over cosmological timescales. Her context is the impending redefinition of the kilogram and other units in terms of fundamental constants – a practice which is seen as more “objective” than defining units in terms of human artefacts. She focusses on one particular constant, the fine structure constant (α), for which some evidence of such a variation has been reported. Although α is not one of the fundamental constants involved in the proposed redefinitions, it is linked to some which are, so that there is a clear cause for concern. One of the authors she references is Michael Duff, who presents an argument supporting his assertion that dimensionless constants are more fundamental than dimensioned ones; this argument employs various systems of so-called “natural units”. [see Riordan (2015); Duff (2004)] An interesting feature of this discussion is that not only Riordan herself, but all the papers she cites, use a formula for α that is valid only in certain systems of units, and would not feature in a modern physics textbook. This violates another aspect of objectivity – namely, the idea that our physical laws should be expressed in such a way that they are independent of the particular units we choose to use; they should be unit-invariant. In this paper I investigate the place of unit-invariance in the history of physics, together with its converse, unit-dependence, which we will find is a common feature of some branches of physics, despite the fact that, as I will show in an analysis of Duff’s argument, unit-dependent formulae can lead to erroneous conclusions.
    [Show full text]
  • FORMAT Bulletin
    Members’ Paper From IRPS Bulletin Vol 10 No 3 September/October, 1996 ONE HUNDRED YEARS OF ELECTRONS above hypothesis but also to the brilliant discoveries made in the closing years of the 19th century: that of X- Leif Gerwarda and Christopher Cousinsb rays by Wilhelm Conrad Röntgen in 1895 and that of radioactivity by Henri Becquerel in 1896. a. Department of Physics, Technical University of Denmark, Lyngby, Denmark Cathode rays occurs when electricity is discharged in a rarefied gas. At a given low pressure of the gas, rays are b. Department of Physics, University of Exeter, emitted from the negative pole, the cathode. The Exeter, UK cathode rays themselves are invisible, but they can be observed by the phosphorescence that they induce at the The search for the true nature of electricity led walls of the glass tube and by the shadows from objects to the discovery of the electron and the proof placed in their path. The cathode rays propagate in that it is a constituent of all atoms. These straight lines, but unlike ordinary light rays they can be achievements gave the scientists the first deflected by a magnetic field. definite line of attack on the constitution of the atom and on the structure of matter. The phenomena exhibited by the electric discharge in rarefied gas had long been familiar from studies by In a lecture on 'The Stability of Atoms' given to the Royal Julius Plücker, Wilhelm Hittorf, Eugen Goldstein and Society of Arts in 1924, Ernest Rutherford said: other physicists. In a lecture delivered before the British Association at the Sheffield Meeting in 1879, William The trend of physics during the past twenty-five years has Crookes first used the expression radiant matter or been largely influenced by three fundamental discoveries matter in the ultra-gaseous state, to explain the made in the closing years of the nineteenth century.
    [Show full text]
  • Elementary Charge and Electron: One Entity Two Identities
    Preprints (www.preprints.org) | NOT PEER-REVIEWED | Posted: 27 April 2021 doi:10.20944/preprints202104.0716.v1 Elementary Charge and Electron: One Entity Two Identities MISHECK KIRIMI1, 2 1. Department of Health Sciences, Moi University, Eldoret, Kenya 2. email: [email protected], [email protected] Our knowledge of electricity is based on two nearly parallel concepts – charge and electron. The charge concept is symmetrical: nature has equal numbers of positive and negative charges playing equivalent roles in atoms. The electron concept has two asymmetries. One, the observable universe has more positive than negative electrons. Two, atoms contain negative- but no positive electrons. Here I propose that charge is static electron and electron is moving charge. That is, resting (electrostatic) and moving (electrodynamic) behaviours exclusively make charge and electron different. The proposal reveals previously unnoticed symmetries in the electron concept and has experimental backing. Faraday, Stoney and Millikan observed charges in static conditions – electrolytes, oil drops, doorknobs etc. In contrast, Thomson and Anderson observed electrons at high speeds in cathode tubes and cloud chambers. Beta decays were initially interpreted to mean existence of electrons in atomic nuclei. Equating ‘charge’ to ‘static electron’ reinstates and validates the interpretation. Key words: Charge, electricity, electron, electrodynamics, electrostatics, elementary charge George Thomson observed that electron “can never be separated” from its charge1. This fact is unique to the electron. Other charged particles do lose their charge. Proton, for example, loses its positive charge in β+ decay2. In contrast, electron does not decay to anything simpler3. Thus, nature has no chargeless (electrically neutral) electron.
    [Show full text]
  • Electrons 195 Secondary Literature
    Electrons 195 Secondary Literature 29. R. Loudon: The quantum theory of light (Oxford University Press, Oxford 2000) 30. The Feynman Lectures on Physics (Addison-Wesley 2005, Vol. 3) 31. J.C.H. Spence: Lensless (Diffractive) Imaging, in: Science of Microscopy.P.Hawkes, J.C.H. Spence Eds. (Springer, Berlin 2007, Ch. 19) E Electrons Theodore Arabatzis The discovery of the electron was a complex and extended process, stretching from Faraday’s investigation of electrolysis to Millikan’s oil-drop experiments [18]. The results of four different fields (electrochemistry, electromagnetic theory, spec- troscopy,and cathode rays) converged to support the existence of a novel subatomic constituent of matter. Faraday’s experiments on electrolysis, interpreted from the perspective of the atomic theory of matter, implied that electricity has an atomic structure [4]. That is, electricity appears in naturally occurring units. In 1891 George Johnstone Stoney (1826–1911) named those units “electrons” ( [13], p. 583, [30]). In 1894 Stoney’s electrons were appropriated by Joseph Larmor (1857–1942) to overcome certain empirical and conceptual problems faced by Maxwell’s electro- magnetic theory ([6], pp. 806 ff.). Larmor’s electrons were supposed to be universal constituents of matter and were represented as structures in the all-pervading ether. On the continent a similar electromagnetic theory had been proposed by Hendrik Antoon Lorentz (1853–1928), who developed a synthesis of British and Continental traditions in electromagnetism [7]. Lorentz’s theory incorporated Maxwell’s sug- gestion that electromagnetic phenomena are wave processes in the ether and the suggestion of continental theorists (e.g., Wilhelm Weber) that these phenomena are due to the action of charged particles.
    [Show full text]
  • The History of Stellar Photometry
    The History of Stellar Photometry Downloaded from https://www.cambridge.org/core. IP address: 170.106.202.58, on 25 Sep 2021 at 17:46:06, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms. https://doi.org/10.1017/S0252921100007326 George M. Minchin, FRS (1845-1914) William H.S. Monck (1839-1915) George F. Fitzgerald, FRS (1851-1901) Stephen M. Dixon (1866-1940) Downloaded from https://www.cambridge.org/core. IP address: 170.106.202.58, on 25 Sep 2021 at 17:46:06, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms. https://doi.org/10.1017/S0252921100007326 at^sa^^ii^^^^^-^^^jijfiigjj Biographical and Historical Notes on the Pioneers of Photometry in Ireland The Editors Introduction As the circumstances of the early electrical measurements of starlight in Ireland are not widely known we wish to take this opportunity to set down the facts, as far as they are known to us. Corrections or new information will be welcomed. The observations made in Dublin in 1892 were the result of a collaboration be­ tween four graduates of Trinity College: George M. Minchin, William H.S. Monck, Stephen M. Dixon and George F. Fitzgerald. The observations in 1895 were made at Daramona Observatory, Co. Westmeath with a 24-inch reflector by Minchin, Fitzger­ ald and the owner of the telescope, William E. Wilson. In 1875 Minchin was appointed Professor of Applied Mechanics at the Royal Indian Engineering College at Coopers Hill, near Staines in London. In 1877 he started a long series of investigations of photoelectricity using a small optical laboratory at Coopers Hill and the laboratories of University College London.
    [Show full text]
  • Electron-A Main Actor in Scientific Controversies
    ORG ANON 41:2009 Isabel Serra (Lisbon, Portugal) - Francisco Viegas (Lisbon, Portugal) - Elisa Maia (Lisbon, Portugal) ELECTRON - A MAIN ACTOR IN SCIENTIFIC CONTROVERSIES* 1. Introduction The story of the electron can contribute to the study of the continuity- discontinuity of the scientific thinking in modern age as well as to discussions of models and metaphors in the history of science. Actually, the electron played a central role in several scientific controversies: the nature of elec- tricity and cathode rays, structure and properties of matter. The idea of an atom of electricity was introduced by Michael Faraday (1791-1867) and adopted by Hermann von Helmholtz (1821-1894). In 1874, Johnstone Stoney (1826-1911) estimated its charge and named it electron. However, James Clerk Maxwell (1831-1879) had stated that a complete knowledge of electricity would eliminate the necessity of such particles. The controversy about the nature of electricity lied dormant for years until it was brought to light by the study of discharges in gases. The nature of cathode rays divided physicists and chemists, with the electron playing the major role in the dispute. The experiences of Jean Baptiste Perrin (1870-1942) in 1895 and Joseph John Thomson (1856-1940) in 1897 seemed to confirm the existence of the electron, but did not convince all scientists. The electron became the main protagonist of a controversial image of matter: the atomistic view. In 1913 Niels Bohr's (1885-1962) atomic theory was received with enthusiasm by some physicists but with criticism by others. Nevertheless, the atomic structure of matter gradually wins acceptance by reason of its extraord- inary power in predicting spectral lines.
    [Show full text]
  • George Francis Fitzgerald 1851 - 1901
    George Francis Fitzgerald 1851 - 1901 George Francis Fitzgerald was the leader of the Maxwellians, an "invisible college" of eminent physicists who perfected Maxwell's theory and applied it widely. They included Lodge, Larmor, Heaviside, Hertz and Thomson (JJ, but not Kelvin, who remained sceptical). Together they developed the theory of electromagnetism, in which light is seen as an electromagnetic wave. He was born into the intellectual community of Trinity College, Dublin, where his father was a professor. His uncle George Johnstone Stoney coined the name "electron ". Eventually he was to marry the daughter of the Provost, who was also a physicist. He had the makings of an establishment figure but temperamentally he was a restless spirit, challenging authority and lamenting the old fashioned ways of his academic colleagues, especially in later life. To his colleagues in research he was a generous and imaginative correspondent and he was an outspoken advocate of scientific education and research. A consequence of relativity theory is the apparent shortening of a body due to its motion relative to the observer Today his name is mainly associated with the Fitzgerald contraction in Relativity. This is the apparent shortening of a body due to its motion relative to the observer. The idea came upon him when he was sitting with his friend Oliver Lodge in Liverpool. Characteristically, he published it only as an obscure note in a minor American journal. He was embarrassed when Hendrik Lorentz later had the same idea. Both names are now attached to this effect. Fitzgerald's interests extended to practical physics. In 1895 he purchased the new Lilienthal glider and flew it (at a prudently low altitude, and still wearing his top hat) in the college grounds, towed by a team of students and enduring the sarcasm of the Dublin citizenry, who looked on in amazement through the railings.
    [Show full text]
  • What Is Electron?
    What is electron? In Gee Kim GIFT, POSTECH December 5, 2013 Contents History and Discovery Fundamental properties Free relativistic quantum fields Free field quantizations Electromagnetic interaction Renomalization Renormalization Group and Higgs mechanism Summary History 1600 De Magnete (William Gilbert): new L. electricus, L. < electrum, Gk. < ηλεκτρoν¯ , amber. 1838 Richard Laming: P Atom = core matter + surrounding (unit electric charge). 1846 William Weber: Electricity = P fluid(+) + P fluid(−) . 1881 Hermann von Helmholtz: “behaves like atoms of electricity.” 1891 George Johnstone Stoney: electron = electr(ic) + (i)on. Discovery Crookes tube: 1869 Johann Wilhelm Hittorf: A glow emitted from the cathode. 1876 Eugen Goldstein: Cathode rays. 1870 Sir William Crookes: The luminescence rays comes from the cathod rays which I carried energy, I moved from cathod to anode, and I bent in magnetic field as negative charged. 1890 Arthur Schuster: The charge-to-mass ratio, e=m Discovery 1892 Hendrik Antoon Lorentz: mass ( electric charge. 1896 J. J. Thomson with John S. Townsend and H. A. Wilson: e=m was independent of cathode material. 1896 George F. Fitzgerald: The universality of e=m and again proposed the name electron. 1896 Henri Becquerel: Radioactivity. 1896 Ernest Rutherford designated the radioactive particles, alpha (α) and beta (β). 1900 Becquerel: The β-rays have the same e=m as electrons. 1909 Robert Millikan and Harvey Fletcher: The oil-drop experiments (published in 1911). 1913 Abram Ioffe confirmed the Millikan’s experiments. Fundamental properties Mass: m = 9:109 × 10−31 kg = 0:511 MeV=c2, where c = 2:998 × 108 m=s. Charge: e = −1:602 × 10−19 C Spin: Intrinsic spin angular momentum with 2 2 I S = s(s + 1)~ , the square of the spin magnitude, 1 h −34 where s = ± 2 and ~ = 2π = 1:0546 × 10 Js.
    [Show full text]
  • On Our Way to Redefine the Base Units Solely from Fundamental Constants
    Reforming the international system of units: On our way to rede…ne the base units solely from fundamental constants and beyond Ch.J. Bordé Laboratoire de Physique des Lasers, UMR 7538 CNRS, Université Paris Nord, 99 avenue J.-B. Clément, 93430 Villetaneuse, France LNE-SYRTE, UMR 8630 CNRS, Observatoire de Paris 61 avenue de l’Observatoire, 75 014 Paris, France Abstract Thanks to considerable progress in quantum technologies, the trend today is to rede…ne all SI base units from fundamental constants and we discuss strategies to achieve this goal. We …rst outline the present situation of each of the seven base units and examine the choice of fundamental constants which can reasonably be …xed. A critical issue is how we should rede…ne the unit of mass in the con- text of modern relativistic quantum theory. At the microscopic level the link of mass with proper time as conjugate variables in the quan- tum phase S=~ is well established. This link strongly suggests that we should …x the value of Planck’s constant h, thus de…ning mass through a de Broglie-Compton frequency mc2=h. This frequency can be accurately measured for atomic and molecular species by atom interferometry. The main di¢ culty is then to bridge the gap with the macroscopic scale for which phases are usually scrambled by decoher- ence and where all mechanical quantities are built from the classical action S only without connexion to a quantum phase. Two ways are now being explored to make this connexion: either the electric kilogram which uses recent progress in quantum electrical metrol- ogy or atom interferometry combined with the Avogadro number determination using a silicon sphere.
    [Show full text]
  • Stoney's Electron
    HISTORY OF PHYSICS 159 and accordingly he quoted that committee in determining that an Ampère-second (or Stoney's Coulomb) causes dissociation of 92 x to 6 gm of H20. With oxygen having atomic weight 16 and hydrogen atomic weight 1, Electron Stoney estimated that this quantity of Patrick A.Wayman water would contain: 92 x 1o-6 x (2/16) x Dublin Institute for Advanced Studies (1/1025) = x.15 x 1020 H atoms. Rounding this to 1020, Stoney deduced George Johnstone Stoney, the man who that one chemical bond would correspond named the electron, was led to the concept to 1o-20 Coulombs (which he calls of a fundamental unit of electric charge by Ampères). However, without dropping a combining electro-chemistry with the factor of 2, as explained above, and withou kinetic theory of gases. But his understand­ other approximation, he could have ing was incomplete (so the discovery of the arrived at the figure of 4.35 x 1o-21 electron is associated with JJ Thomson's Coulombs for his ‘unit of charge’. determination of its charge to mass ratio in The latter figure, as compared with a October 1897) modern figure for the charge on the elec­ The suggestion of the name ‘electron’ Stoney was able, by the 1870s, to com­ tron of 1.6018 x 1019 Coulombs, is low by a (amber in Greek) for a hypothetical small prehend a unit of electric charge being factor of 36.8 (not 16 as was 1o-20). In unit of electric charge is generally attrib­ exchanged in electro-chemical processes tracking down this discrepancy we notice uted to George Johnstone Stoney, FRS, involving molecules of water.
    [Show full text]