John Randall (physicist)

Sir John Turton Randall
Born 23 March 1905
Newton-le-Willows, Lancashire, England
Died 16 June 1984(1984-06-16) (aged 79)
Residence United Kingdom
Fields Experimental physicist and biophysicist
Institutions GEC, The Cavendish Laboratory of the University of Cambridge, King's College, London, University of St Andrews, University of Birmingham, and Dept. of Zoology at the University of Edinburgh
Alma mater University of Manchester and The Cavendish Laboratory of the University of Cambridge
Doctoral advisor Nobel-prize winner, Sir-William Lawrence Bragg, Head of The Cavendish Laboratory
Doctoral students 49
Known for High-power, multi-cavity magnetron for British and American radar stations in WWII, DNA structure determination, neutron diffraction studies of labelled proteins
Notable awards Duddell Medal and Prize (1945)
Hughes Medal (1946)
FRSE
John Price Wetherill Medal (1958)
Fellow of the Royal Society[1]

Sir John Turton Randall, FRS, FRSE (23 March 1905 – 16 June 1984) was a British physicist and biophysicist, credited with radical improvement of the cavity magnetron, an essential component of centimetric wavelength radar, which was one of the keys to the Allied victory in the Second World War. It is also the key component of microwave ovens. He also led the King's College, London team which worked on the structure of DNA; his deputy, Professor Maurice Wilkins, shared the 1962 Nobel Prize for Physiology or Medicine, together with James Watson and Francis Crick of the Cavendish Laboratory at the University of Cambridge, for the determination of the structure of DNA. His other staff included Rosalind Franklin, Raymond Gosling, Alex Stokes and Herbert Wilson, all involved in research on DNA.

Origins

John Randall was born on 23 March 1905 at Newton-le-Willows, Lancashire, the only son and the first of the three children of Sidney Randall, nurseryman and seedsman, and his wife, Hannah Cawley, daughter of John Turton, colliery manager in the area.[1] He was educated at the grammar school at Ashton-in-Makerfield and at the University of Manchester, where he was awarded a first-class honours degree in physics and a graduate prize in 1925, and an MSc in 1926. He married Doris, daughter of Josiah John Duckworth, a colliery surveyor, in 1928.[1] They had one son, Christopher, born in 1935.[1]

From 1926 to 1937 Randall was employed on research by the General Electric Company at its Wembley laboratories, where he took a leading part in developing luminescent powders for use in discharge lamps. He also took an active interest in the mechanisms of such luminescence.[1]

By 1937 he was recognised as the leading British worker in his field, and was awarded a Royal Society fellowship to the University of Birmingham, where he worked on the electron trap theory of phosphorescence in Professor Marcus Oliphant's physics faculty.[2]

The Magnetron

Poynting Physics Building, Birmingham University
An original six-cavity magnetron.

When the war began in 1939, Oliphant was approached by the Admiralty about the possibility of building a radio source that operated at microwave frequencies. Such a system would allow a radar using it to see small objects like the periscopes of submerged U-boats. The Air Ministry radar researchers at Bawdsey Manor had also expressed an interest in a 10 cm system, as this would greatly reduce the size of the transmission antennas, making them much easier to fit in the nose of aircraft, as opposed to being mounted on the wings and fuselage as in their current systems.[3]

Oliphant began research using the klystron, a device introduced by Russell and Sigurd Varian between 1937 and 1939, and the only system known to efficiently generate microwaves. Klystrons of the era were very low-power devices, and Oliphant's efforts were primarily directed to greatly increasing their output. If this were successful, it created a secondary problem; the klystron was an amplifier only, so a low-power source signal was needed for it to amplify. Oliphant put Randall and Harry Boot on this issue of producing a microwave oscillator, asking them to explore miniature Barkhausen–Kurz tubes for this role, a design already used for UHF systems. Their work quickly demonstrated that these offered no improvement in the microwave range.[4] The klystron effort soon plateaued with a device that could generate about 400 watts of microwave power, enough for testing purposes, but far short of the multi-kilowatt systems that would be required for a practical radar system.

Randall and Boot, given no other projects to work on, began considering solutions to this problem in November 1939. The only other microwave device known at that time was the split-anode magnetron, a device capable of generating small amounts of power, but with low efficiency and generally lower output than the klystron. However, they noted that it had one enormous advantage over the klystron; the klystron's signal is encoded in a stream of electrons provided by an electron gun, and it was the current capability of the gun that defined how much power the device could ultimately handle. In contrast, the magnetron used a conventional hot filament cathode, a system that was widely used in radio systems producing hundreds of kilowatts. This seemed to offer a much more likely path to higher power.[4]

The problem with existing magnetrons was not power, but efficiency. In the klystron, a beam of electrons was passed through a metal disk known as a resonator. The mechanical layout of the copper resonator caused it to influence the electrons, speeding them up and slowing them down, releasing microwaves. This was reasonably efficient, and power was limited by the guns. In the case of the magnetron, the resonator was replaced by two metal plates held at opposite charges to cause the alternating acceleration, and the electrons were forced to travel between them using a magnet. There was no real limit to the number of electrons this could accelerate, but the microwave release process was extremely inefficient.

The two then considered what would happen if the two metal plates of the magnetron were replaced by resonators, essentially combining the existing magnetron and klystron concepts. The magnet would cause the electrons to travel in a circle, as in the case of the magnetron, so they would pass by each of the resonators, generating microwaves much more efficiently than the plate concept. Recalling that Heinrich Hertz had used loops of wire as resonators, as opposed to the disk-shaped cavities of the klystron, it seemed possible that multiple resonators could be placed around the centre of the magnetron. More importantly, they was no real limit to the number or size of these loops. One could greatly improve the power of the system by extending the loops into cylinders, the power handling then being defined by the length of the tube. Efficiency could be improved by increasing the number of resonators, as each electron could thus interact with more resonators during its orbits. The only practical limits were based on the required frequency and desired physical size of the tube.[4]

Developed using common lab equipment, the first magnetron consisted of a copper block with six holes drilled through it to produce the resonant loops, which was then placed in a bell jar and vacuum pumped, which was itself placed between the poles of the largest horseshoe magnet they could find. A test of their new cavity magnetron design in February 1940 produced 400 watts, and within a week it had been pushed over 1.000 watts.[4] The design was then demonstrated to engineers from GEC, who were asked to try to improve it. GEC introduced a number of new industrial methods to better seal the tube and improve vacuum, and added a new oxide-coated cathode that allowed for much greater currents to be run through it. These boosted the power to 10 kW, about the same power as the conventional tube systems used in existing radar sets. The success of the magnetron revolutionised the development of radar, and almost all new radar sets from 1942 on used one.

In 1943 Randall left Oliphant's physical laboratory in Birmingham to teach for a year in the Cavendish Laboratory at Cambridge. In 1944 Randall was appointed professor of natural philosophy at University of St Andrews and began planning research in biophysics (with Maurice Wilkins) on a small Admiralty grant.[5]

King's College, London

In 1946, John T Randall – who had as PhD advisor the Nobel Prize–winning physicist, William Lawrence Bragg – was appointed Head of Physics Department at King's College in London. He then moved to the Wheatstone chair of physics at King's College, London, where the Medical Research Council set up the Biophysics Research Unit with Randall as the director (now known as Randall Division of Cell and Molecular Biophysics) at King's College. During his term as Director the experimental work leading to the discovery of the structure of DNA was made there by Rosalind Franklin, Raymond Gosling, Maurice Wilkins, Alex Stokes and Herbert R. Wilson. He assigned Raymond Gosling as a PhD student to Dr. R. Franklin to work on DNA structure by X-ray diffraction.[6] According to Raymond Gosling, the role of John Randall in the pursuit of the double helix cannot be overstated. Gosling felt so strongly on this subject that he wrote to The Times in 2013 during the sixtieth anniversary celebrations.[7] Randall firmly believed that DNA held the genetic code and assembled a multi-disciplinary team to help prove it. It was Randall who pointed out that since DNA was largely carbon, nitrogen and oxygen, it was just the same as the atoms in the air in the camera. The result was a diffuse back-scattering of X-rays, which fogged the film, and so he instructed Gosling to displace all the air with hydrogen.[7]

Maurice Wilkins shared the 1962 Nobel Prize for Physiology and Medicine with James Watson and Francis Crick; Rosalind Franklin had already died from cancer in 1958.

In addition to the X-Ray diffraction work the unit conducted a wide-ranging programme of research by physicists, biochemists, and biologists. The use of new types of light microscopes led to the important proposal in 1954 of the sliding filament mechanism for muscle contraction. Randall was also successful in integrating the teaching of biosciences at King's College.[1]

In 1951 he set up a large multidisciplinary group working under his personal direction to study the structure and growth of the connective tissue protein collagen. Their contribution helped to elucidate the three-chain structure of the collagen molecule. Randall himself specialised in using the electron microscope, first studying the fine structure of spermatozoa and then concentrating on collagen.[1] In 1958 he published a study of the structure of protozoa.[1] He set up a new group to use the cilia of protozoa as a model system for the analysis of morphogenesis by correlating the structural and biochemical differences in mutants.

Later years

In 1970 he retired to Edinburgh University, where he formed a group which applied a range of new biophysical methods, such as coherent neutron diffraction studies of protein crystals in ionic solutions in heavy water, to study by neutron diffraction and scattering various biomolecular problems, such as the proton exchange of protein residues by deuterons.

Honours

University of Birmingham – Poynting Physics Building – blue plaque

Books featuring Sir John Randall, FRSE

See also

Notes

  1. 1 2 3 4 5 6 7 8 9 10 Wilkins, M. H. F. (1987). "John Turton Randall. 23 March 1905 – 16 June 1984". Biographical Memoirs of Fellows of the Royal Society 33: 492–426. doi:10.1098/rsbm.1987.0018. JSTOR 769961. PMID 11621437.
  2. ↑ J. T. Randall, M. H. F. Wilkins, "The Interpretation of Long-Period Phosphorescence", Proceedings of the Royal Society, DOI: 10.1098/rspa.1945.0025, 6 November 1945
  3. ↑ Bowen 1998, p. 143.
  4. 1 2 3 4 Randal and Boot, "Historical Notes on the Cavity Magnetron", IEEE, July 1976, p. 724.
  5. ↑ "The cell: dissecting the new anatomy". King's College London.
  6. ↑ See the letter sent from Randall to Franklin.
  7. 1 2 "Raymond Gosling: the man who crystallized genes". Genome Biology 14: 402. 25 April 2013. doi:10.1186/gb-2013-14-4-402. Retrieved 8 May 2013.

External links

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