John James Waterston

John James Waterston (1811 – 18 June 1883) was a Scottish physicist, a neglected pioneer of the kinetic theory of gases.

Early life

Waterston's father, George, was an Edinburgh sealing wax manufacturer and stationer, a relative of the Sandeman family Robert and his brother, George. John was born, the sixth of nine children, into a family alive with interests in literature, science and music. He was educated at Edinburgh High School before becoming apprenticed as a civil engineer to Messrs. Grainger and Miller. His employers encouraged him to attend lectures at the University of Edinburgh. He studied mathematics and physics under Sir John Leslie as well as attending lectures in chemistry, anatomy and surgery and becoming an active participant in the student literary society.

At age nineteen, Waterston published a paper proposing a mechanical explanation of gravitation, accounting for action at a distance in terms of colliding particles and discussing interactions between linear and rotational motion that would play a part in his later kinetic theory.

Waterston moved to London at age twenty-one, where he worked as a railroad surveyor, becoming an associate of the Institution of Civil Engineers and publishing a paper on a graphical method for planning earthworks. The travel and disruption associated with his surveying work left Waterston little time to pursue his studies so he joined the hydrography department of the Admiralty under Francis Beaufort. It was Beaufort who, in 1839, supported Waterston for the post of naval instructor for cadets of the East India Company in Bombay. The posting worked well for Waterston who was able to pursue his reading and research at the library of Grant College.

Kinetic theory

While in India, he first developed his kinetic theory, independently of earlier and equally neglected partial accounts by Daniel Bernoulli and John Herapath. He published it, at his own expense, in his book Thoughts on the Mental Functions (1843). He correctly derived all the consequences of the premise that gas pressure is a function of the number of molecules per unit volume, N; molecular mass, M; and molecular mean-squared velocity, . He established the relationship:

.

He had been motivated to think of a wave theory of heat by analogy with the wave theory of light and some experiments by James Forbes and Macedonio Melloni on radiant heat. His statement that ... in mixed media the mean square molecular velocity is inversely proportional to the specific weight of the molecules has been seen as the first statement of the equipartition theorem for translational motion. Waterston grasped that, while the kinetic energy of an individual molecule with velocity v is ½mv², heat energy is proportional to temperature, T. That insight led him to derive the ideal gas law:

.

The publication made little impact, perhaps because of the title. He submitted his theory, under Beaufort's sponsorship, to the Royal Society in 1845 but was rejected. Referee Sir John William Lubbock wrote The paper is nothing but nonsense.

Unable to retrieve a copy of his paper (he had failed to make a copy for himself before submitting the paper to the Royal Society), he rewrote the work and sought to advertise it elsewhere, attracting little attention other than from William John Macquorn Rankine and Hermann von Helmholtz through whom it may have influenced August Krönig. The theory gained acceptance only when it was proposed by Rudolf Clausius and James Clerk Maxwell in the 1850s by which time Waterston's contribution had been forgotten.

Later life

He returned to Edinburgh in 1857 to pursue his own novel physical ideas but met with unyielding neglect and discouragement from the scientific establishment. Neglect was exacerbated by his own increasing reclusiveness and hostility to the learned societies. He worked on acoustics, astronomy, fluid mechanics and thermodynamics.

He left his Edinburgh home on 18 June and drowned in a nearby canal, possibly falling into the canal due to heat stress from his astronomical observation activities.[1]

Recognition after death

As discussed above, Waterston's paper submitted to the Royal Society was rejected. Some years after Waterston's death, Lord Rayleigh (Secretary of Royal Society at that time) managed to dig it out from the archives of the Royal Society. Finally, Waterson's paper was published in the Philosophical Transactions of the Royal Society in 1892. (Please see below.)

Rayleigh felt that Waterston's case was not an aberration, but the norm:[2]

"The history of [Waterston's] paper suggests that highly speculative investigations, especially by an unknown author, are best brought before the world through some other channel than a scientific society, which naturally hesitates to admit into its printed records matter of uncertain value. Perhaps one may go further, and say that a young author who believes himself capable of great things would usually do well to secure favourable recognition of the scientific world by work whose scope is limited, and whose value is easily judged, before embarking upon higher flights."

John Herapath

John Herapath was another contemporaneous English physicist who also worked on the kinetic theory, and whose work was also neglected at the time.

References

  1. ↑ How Astronomers Die, a presentation by Historian Thomas Hockey
  2. ↑ Duncan, Ronald F. H. and M. Weston-Smith (eds.) (1979). "(Lord Rayleigh Cited by R. A. Lyttleton in the chapter, The Gold Effect)". Lying Truths: A Critical Scrutiny of Current Beliefs and Conventions. Oxford: Pergamon. p. 194. ISBN 978-0080219783.

Bibliography

External links

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