G. I. Taylor

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Sir Geoffrey Ingram Taylor
G I Taylor.jpg
Sir Geoffrey Ingram Taylor
Born (1886-03-07)7 March 1886
St. John's Wood, London
Died 27 June 1975(1975-06-27) (aged 89)
Cambridge
Nationality British
Fields Physics
Mathematics
Fluid mechanics
Fluid dynamics
Solid mechanics
Wave theory
Alma mater Trinity College, Cambridge
Academic advisors J. J. Thomson[1][2]
Doctoral students George Batchelor
Walter Freiberger
Known for Taylor cone
Taylor dispersion
Taylor number
Taylor vortex
Taylor–Couette flow
Taylor–Goldstein equation
Rayleigh–Taylor instability
Taylor–Proudman theorem
Taylor–Green vortex
Taylor microscale
Taylor column
Notable awards Knight Bachelor
Royal Medal (1933)
Copley Medal (1944)
Order of Merit
De Morgan Medal (1956)
Timoshenko Medal (1958)
Franklin Medal (1962)
FRS[3]
Theodore von Karman Medal (1969)

Sir Geoffrey Ingram Taylor OM (7 March 1886 – 27 June 1975) was a British physicist and mathematician, and a major figure in fluid dynamics and wave theory. His biographer and one-time student, George Batchelor, described him as "one of the most notable scientists of this (the 20th) century".[3][4][5][6][7][8]

Biography[edit]

Taylor was born in St. John's Wood, London. His father, Edward Ingram Taylor, was an artist, and his mother, Margaret Boole, came from a family of mathematicians (his aunt was Alicia Boole Stott and his grandfather was George Boole). As a child he was fascinated by science after attending the Royal Institution Christmas Lectures, and performed experiments using paint rollers and sticky-tape. Taylor followed in his grandfather's footsteps, reading mathematics at Trinity College, Cambridge.

His first paper was on quanta showing that Young's slit diffraction experiment produced fringes even with feeble light sources such that less than one photon on average was present at a time. He followed this up with work on shock waves, winning a Smith's Prize. In 1910 he was elected to a Fellowship at Trinity College, and the following year he was appointed to a meteorology post, becoming Reader in Dynamical Meteorology. His work on turbulence in the atmosphere led to the publication of "Turbulent motion in fluids", which won him the Adams Prize in 1915.

In 1913 Taylor served as a meteorologist aboard the Ice Patrol vessel Scotia, where his observations formed the basis of his later work on a theoretical model of mixing of the air. At the outbreak of World War I, he was sent to the Royal Aircraft Factory at Farnborough to apply his knowledge to aircraft design, working, amongst other things, on the stress on propeller shafts. Not content just to sit back and do the science, he also learned to fly aeroplanes and make parachute jumps.

After the war Taylor returned to Trinity and worked on an application of turbulent flow to oceanography. He also worked on the problem of bodies passing through a rotating fluid. In 1923 he was appointed to a Royal Society research professorship as a Yarrow Research Professor. This enabled him to stop teaching, which he had been doing for the previous four years, and which he both disliked and had no great aptitude for. It was in this period that he did his most wide-ranging work on fluid mechanics and solid mechanics, including research on the deformation of crystalline materials which followed from his war work at Farnborough. He also produced another major contribution to turbulent flow, where he introduced a new approach through a statistical study of velocity fluctuations.

In 1934, Taylor, roughly contemporarily with Michael Polanyi and Egon Orowan, realised that the plastic deformation of ductile materials could be explained in terms of the theory of dislocations developed by Vito Volterra in 1905. The insight was critical in developing the modern science of solid mechanics.

During World War II, Taylor again applied his expertise to military problems such as the propagation of blast waves, studying both waves in air and underwater explosions. Taylor was sent to the United States in 1944–1945 as part of the British delegation to the Manhattan Project. At Los Alamos, Taylor helped solve implosion instability problems in the development of atomic weapons.

In 1944 he also received his knighthood and the Copley Medal from the Royal Society.

Taylor continued his research after the war, serving on the Aeronautical Research Committee and working on the development of supersonic aircraft. Though he officially retired in 1952, he continued research for the next twenty years, concentrating on problems that could be attacked using simple equipment. This led to such advances as a method for measuring the second coefficient of viscosity. Taylor devised an incompressible liquid with separated gas bubbles suspended in it. The dissipation of the gas in the liquid during expansion was a consequence of the shear viscosity of the liquid. Thus the bulk viscosity could easily be calculated. His other late work included the longitudinal dispersion in flow in tubes, movement through porous surfaces, and the dynamics of sheets of liquids.

Aspects of Taylor's life often found expression in his work. His over-riding interest in the movement of air and water, and by extension his studies of the movement of unicellular marine creatures and of weather, were related to his lifelong love of sailing. In the 1930s he invented the 'CQR' anchor, which was both stronger and more manageable than any in use, and which was used for all sorts of small craft including seaplanes.[9]

His final research paper was published in 1969, when he was 83. In it he resumed his interest in electrical activity in thunderstorms, as jets of conducting liquid motivated by electrical fields. The cone from which such jets are observed is called the Taylor cone for him. In the same year Taylor received the A. A. Griffith Medal and Prize and was appointed to the Order of Merit. He suffered a stroke in 1972 which effectively put an end to his work; he died in Cambridge in 1975.

References[edit]

  1. ^ O'Connor, John J.; Robertson, Edmund F., "G. I. Taylor", MacTutor History of Mathematics archive, University of St Andrews .
  2. ^ G. I. Taylor at the Mathematics Genealogy Project
  3. ^ a b Batchelor, G. K. (1976). "Geoffrey Ingram Taylor 7 March 1886 -- 27 June 1975". Biographical Memoirs of Fellows of the Royal Society 22: 565. doi:10.1098/rsbm.1976.0021.  edit
  4. ^ G. K. Batchelor, The Life and Legacy of G. I. Taylor (1994), p. 1. ISBN 0-521-46121-9
  5. ^ The Life and Legacy of G. I. Taylor, by George Batchelor, Cambridge University Press, 1994 ISBN 0-521-46121-9
  6. ^ Taylor, Geoffrey Ingram, Sir, Scientific papers. Edited by G.K. Batchelor, Cambridge University Press 1958–71. (Vol. 1. Mechanics of solids – Vol. 2. Meteorology, oceanography, and turbulent flow – Vol. 3. Aerodynamics and the mechanics of projectiles and explosions – Vol. 4. Mechanics of fluids: miscellaneous papers).
  7. ^ "G.I. Taylor as I Knew Him". "Advances in Applied Mechanics Volume 16". Advances in Applied Mechanics 16. 1976. pp. xii–. doi:10.1016/S0065-2156(08)70086-3. ISBN 9780120020164.  edit
  8. ^ Pippard, S. B. A. (1975). "Sir Geoffrey Taylor". Physics Today 28 (9): 67–61. doi:10.1063/1.3069178.  edit
  9. ^ Taylor, G. I., The Holding Power of Anchors April 1934

External links[edit]