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Rayleigh and Ramsay
Argon ( αργος, Greek meaning " inactive ", in reference to its chemical inactivity ) was suspected to be present in air by Henry Cavendish in 1785 but was not isolated until 1894 by Lord Rayleigh and Sir William Ramsay in Scotland in an experiment in which they removed all of the oxygen, carbon dioxide, water and nitrogen from a sample of clean air.
John William Strutt, 3rd Baron Rayleigh, OM ( 12 November 1842 – 30 June 1919 ) was an English physicist who, with William Ramsay, discovered argon, an achievement for which he earned the Nobel Prize for Physics in 1904.
Along with scientist William Ramsay at University College, London, Lord Rayleigh theorized that the nitrogen extracted from air was mixed with another gas, leading to an experiment that successfully isolated a new element, argon, from the Greek word (, " inactive ").
* Sir William Ramsay and Lord Rayleigh discover the first noble gas, Argon.
Sir William Ramsay ( 1852 – 1916 ) was a Scottish chemist who discovered the noble gases and received the Nobel Prize in Chemistry in 1904 " in recognition of his services in the discovery of the inert gaseous elements in air " ( along with Lord Rayleigh who received the Nobel Prize in Physics that same year for the discovery of argon ).
On the evening of 19 April 1894 Ramsay attended a lecture given by Lord Rayleigh.
By August, Ramsay could write to Rayleigh to announce that he had isolated a heavy component of air, previously unknown, which did not appear to have any obvious chemical reactivity.
* 1894 Lord Rayleigh and William Ramsay discover argon by spectroscopically analyzing the gas left over after nitrogen and oxygen are removed from air
In the 1890s ( around 100 years later ) two British physicists, William Ramsay and Lord Rayleigh, realized that their newly discovered inert gas, argon, was responsible for Cavendish's problematic residue ; he had not made an error.
* Argon identified by Lord Rayleigh and Sir William Ramsay.
The incident of the burning of the library led to a protest note by British scientists, which was signed also by eight distinguished British scientists, namely William Bragg, William Crookes, Alexander Fleming, Horace Lamb, Oliver Lodge, William Ramsay, Baron Rayleigh and J. J. Thomson, and in which it was assumed that the war propaganda mentioned corresponded to real behavior of German soldiers.

Rayleigh and received
* Edward G. S. Paige, Worked on semiconductors, with Denis Maines turned to Surface acoustic wave ( SAW ) devices, led team that received Wolfe Medal of MOD and earned RRE a Queen's Award, later Professor of Electrical Engineering at the University of Oxford, awarded Rayleigh Medal and Duddell Medal,

Rayleigh and 1904
Conceptually different experiments that also attempted to detect the motion of the aether were the Trouton-Noble experiment ( 1903 ) to detect torsion effects caused by electrostatic fields, and the Experiments of Rayleigh and Brace ( 1902, 1904 ) to detect double refraction in various media.
In addition, the Michelson-Morley null result was further substantiated by the null results of other second-order experiments of different kind, namely the Trouton – Noble experiment ( 1903 ) and the Experiments of Rayleigh and Brace ( 1902 – 1904 ).
* Lord Rayleigh ( Physics, 1904 )
Bloembergen belongs to prolific J. J. Thomson academic lineage tree, following in footsteps of other Nobel Laureates beginning with Lord Rayleigh ( Physics Nobel Prize in 1904 ) and J. J. Thomson ( Nobel 1906 ), and continued with Ernest Rutherford ( Nobel Prize in Chemistry 1908 ), Owen Richardson ( Physics Nobel, 1928 ) and finally Bloembergen's advisor, Edward Purcell ( Physics Nobel 1952 ).
: 1902 to 1904 – Lord Rayleigh and DeWitt Bristol Brace found no signs of double refraction ( due to Fitzgerald-Lorentz Contraction ) of moving bodies in the aether.
* Peter Rayleigh, History of Ye Antient Society of Cogers ( London, 1904 ).

Rayleigh and Nobel
* 1842 – John Strutt, 3rd Baron Rayleigh, English physicist, Nobel laureate ( d. 1919 )
* June 30 – John Strutt, 3rd Baron Rayleigh, English physicist, Nobel Prize laureate ( b. 1842 )
* November 12 – John Strutt, 3rd Baron Rayleigh, English physicist, Nobel Prize laureate ( d. 1919 )
Other admirers include physicist Lord Rayleigh and Nobel laureate Philip Anderson.
* John Strutt, 3rd Baron Rayleigh, Nobel Prize winning physicist for the discovery of argon, died in 1919 at Terling Place, Witham.
Instead, he conducted his research with the Nobel Laureate Lord Rayleigh at Cambridge and returned to India.
* June 30-John William Strutt, 3rd Baron Rayleigh ( born 1842 ), Nobel Prize-winning physicist.
* November 12-John William Strutt, 3rd Baron Rayleigh ( died 1919 ), Nobel Prize-winning physicist.

Rayleigh and Physics
* Physics – The Lord Rayleigh
The Physics building opened and the first six floors of Rayleigh tower were ready for occupation, while work began on the Albert Sloman Library.
He hoped to succeed Rayleigh as Cavendish Professor of Physics in 1884, but was surprisingly ( given that he was also Rayleigh's choice ) passed over in favour of Sir J. J. Thomson, which was a great disappointment to him.

Rayleigh and respectively
A generalization of the seminal formulations on constants of motion in Lagrangian and Hamiltonian mechanics ( developed in 1788 and 1833, respectively ), it does not apply to systems that cannot be modeled with a Lagrangian alone ( e. g. systems with a Rayleigh dissipation function ).

Rayleigh and for
John William Strutt, 3rd Baron Rayleigh | Lord Rayleigh's method for the isolation of argon, based on an experiment of Henry Cavendish's.
The Rayleigh Criterion is the basis for analysis of thermoacoustic combustion instability and is evaluated using the Rayleigh Index over one cycle of instability
Geophysical techniques used for subsurface exploration include measurement of seismic waves ( pressure, shear, and Rayleigh waves ), surface-wave methods and / or downhole methods, and electromagnetic surveys ( magnetometer, resistivity, and ground-penetrating radar ).
Rayleigh scattering of sunlight in the atmosphere causes diffuse sky radiation, which is the reason for the blue color of the sky and the yellow tone of the sun itself.
The amount of Rayleigh scattering that occurs for a beam of light depends upon the size of the particles and the wavelength of the light.
The Rayleigh scattering coefficient for a group of scattering particles is the number of particles per unit volume N times the cross-section.
In this case, the Rayleigh scattering intensity for a single particle is given by
Rayleigh scattering is a good approximation of the manner in which light scattering occurs within various media for which scattering particles have a small size parameter.
Contains a good description of the asymptotic behavior of Mie theory for small size parameter ( Rayleigh approximation ).
Rayleigh scattering is a spectroscopic scattering phenomenon that accounts for the color of the sky.
This became clear when plotting the Rayleigh – Jeans law which, while correctly predicting the intensity of long wavelength emissions, predicted infinite total energy as the intensity diverges to infinity for short wavelengths.
However, the stability analyses of the bubble show that the bubble itself undergoes significant geometric instabilities, due to, for example, the Bjerknes forces and Rayleigh – Taylor instabilities.
Typically, for free convection, the average Nusselt number is expressed as a function of the Rayleigh number and the Prandtl number, written as: Nu = f ( Ra, Pr ).
In fluid mechanics, the Rayleigh number for a fluid is a dimensionless number associated with buoyancy driven flow ( also known as free convection or natural convection ).
When the Rayleigh number is below the critical value for that fluid, heat transfer is primarily in the form of conduction ; when it exceeds the critical value, heat transfer is primarily in the form of convection.
The Rayleigh number for the Earth's mantle, due to internal heating alone, Ra < sub > H </ sub > is given by
A Rayleigh number for bottom heating of the mantle from the core, Ra < sub > T </ sub > can also be defined:
Rayleigh fading is a statistical model for the effect of a propagation environment on a radio signal, such as that used by wireless devices.
Rayleigh fading is viewed as a reasonable model for tropospheric and ionospheric signal propagation as well as the effect of heavily built-up urban environments on radio signals.
In his book, Jakes popularised a model for Rayleigh fading based on summing sinusoids.

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