Sir Geoffrey Ingram TaylorOMFRSFRSE (7 March 1886 – 27 June 1975) was a Britishphysicist and mathematician, who made contributions tofluid dynamics andwave theory.
Taylor was born inSt. 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 wasAlicia Boole Stott and his grandfather wasGeorge Boole).[3] As a child he was fascinated by science after attending theRoyal Institution Christmas Lectures, and performed experiments using paint rollers and sticky-tape.
Taylor read mathematics and physics atTrinity College, Cambridge from 1905 to 1908. He won several scholarships and prizes at Cambridge, one of which enabled him to study underJ. J. Thomson.[4]
Taylor published his first paper while he was still an undergraduate. In it, he showed thatinterference of visible light produced fringes even with extremely weak light sources.[5] The interference effects were produced with light from a gas light, attenuated through a series of dark glass plates, diffracting around a sewing needle. Three months were required to produce a sufficient exposure of the photographic plate. The paper does not mention quanta of light (photons) and does not reference Einstein's 1905 paper on the photoelectric effect, but today the result can be interpreted by saying that less than one photon on average was present at a time. Once it became widely accepted in around 1927 that the electromagnetic field was quantized, Taylor's experiment began to be presented in pedagogical treatments as evidence that interference effects with light cannot be interpreted in terms of one photon interfering with another photon—that, in fact, a single photon's probability amplitudes do interfere by going through both slits of a double-slit apparatus. Modern understanding of the subject has shown that the conditions in Taylor's experiment were not sufficient to demonstrate this, because the light source was not a single-photon source, but the experiment was reproduced in 1986 using a single-photon source, and the same result was obtained.[6]
He followed this up with work onshock waves, winning aSmith's Prize.[7]: 43 In 1910 he was elected to a Fellowship at Trinity College, and the following year he was appointed to ameteorology post, becomingReader in Dynamical Meteorology. His work onturbulence in the atmosphere led to the publication of "Turbulent motion in fluids",[8] which won him theAdams Prize in 1915.[9]In 1913 Taylor served as a meteorologist aboard theIce Patrol vesselScotia, where his observations formed the basis of his later work on a theoretical model of mixing of the air.[4]
At the outbreak ofWorld War I, Taylor was sent to theRoyal Aircraft Factory atFarnborough to apply his knowledge to aircraft design, working, amongst other things, on the stress on propeller shafts. He also learned to fly aeroplanes and studied the stability of parachutes.[4]
After the war Taylor returned to Trinity and worked on an application of turbulent flow tooceanography. He also worked on the problem of bodies passing through a rotating fluid. In 1923 he was appointed to aRoyal 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 onfluid mechanics andsolid mechanics, including research on the deformation of crystalline materials which followed from his war work at Farnborough. He also produced another major contribution toturbulent flow, where he introduced a new approach through a statistical study of velocity fluctuations.[4]
In 1934, Taylor, roughly contemporaneously withMichael Polanyi andEgon Orowan, realised that theplastic deformation ofductile materials could be explained in terms of the theory ofdislocations developed byVito Volterra in 1905. The insight was critical in developing the modern science of solid mechanics.[10][11]
In 1936 he presented theRoyal Institution Christmas Lectures, on "Ships".[12] One of these, on "why ships roll in a rough sea", was the first RI Christmas Lecture to be televised, by theBBC.[12][13]
DuringWorld War II, Taylor again applied his expertise to military problems such as the propagation ofblast waves, studying both waves in air andunderwater explosions.[4]
Taylor was sent to the United States in 1944–1945 as part of theBritish delegation to theManhattan Project. AtLos Alamos, Taylor helped solve implosion instability problems in the development of atomic weapons, particularly the plutonium bomb used at Nagasaki on 9 August 1945.[14][15]
In 1944 he also received his knighthood and theCopley Medal from theRoyal Society. He was elected to the United StatesNational Academy of Sciences the following year.[16]
Taylor was present at theTrinity nuclear test, July 16, 1945, as part of GeneralLeslie Groves' "VIP List" of 10 people who observed the test from Compania Hill, about 20 miles (32 km) northwest of the shot tower. By coincidence,Joan Hinton, another direct descendant of the mathematician George Boole, had been working on the same project and witnessed the event in an unofficial capacity. The cousins met at the time but later followed different paths. Joan, strongly opposed to nuclear weapons, defected to Mao's China, while Taylor maintained that political policy was not within the remit of the scientist.[17]
In 1950, he published two papers estimating the yield of the explosion using theBuckingham Pi theorem, and high speed photography stills from that test, bearing timestamps and physical scale of the blast radius, which had been published inLife magazine. He gave two estimates of 16.8 and 23.7 kt, close to the accepted value of 20 kt, which was stillhighly classified at that time.[18]
Taylor continued his research after the war, serving on theAeronautical Research Committee and working on the development ofsupersonic 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 ofviscosity. 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.[11][19]His other late work included the longitudinal dispersion in flow in tubes,[11][20] movement through porous surfaces, and the dynamics of thin sheets of liquids.[11]
Between the ages of 78 and 83, Taylor wrote six papers on electrohydrodynamics. In this work he returned to his interest in electrical activity inthunderstorms, as jets of conducting liquid motivated by electrical fields. The cone from which such jets are observed is called theTaylor cone, after him. He went on to publish two more papers, on additional topics, in 1971 and 1973. In 1972 D. H. MIchael read Taylor's paper, on making holes in a thin sheet of liquid, at the 13th International Conferences for Theoretical and Applied Mechanics in Moscow. Taylor had suffered a stroke and could not attend. He had presented at every one of the previous conferences.[11]
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 includingseaplanes.[21]
Taylor married Grace Stephanie Frances Ravenhill, a school teacher in 1925. They stayed together until Stephanie's death in 1965. Taylor suffered a severe stroke in 1972 which effectively put an end to his work. He died inCambridge in 1975.[11] He is buried in the churchyard ofSt Edward King and Martyr, Cambridge.
Taylor received many awards and honours.[11]
