Rutherford's Alpha Particle Scattering Experiment

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Rutherford's Alpha Particle Scattering Experiment

Rutherford was the world leader in alpha-particle physics. In 1906, at

McGill, he had been the first to detect slight deflections of alphas

on passage through matter. In 1907, he became a professor at the

University of Manchester, where he worked with Hans Geiger. This was

just a year after Rutherford's old boss, J. J. Thomson, had written a

paper on his plum pudding atomic model suggesting that the number of

electrons in an atom was about the same as the atomic number. (Not

long before, people had speculated that atoms might contain thousands

of electrons. They were assuming that the electrons contributed a good

fraction of the atom's mass.)

Rutherford's alpha scattering experiments were the first experiments

in which individual particles were systematically scattered and

detected. This is now the standard operating procedure of particle

physics. Rutherford's partner in the initial phase of this work was

Hans Geiger, who later developed the Geiger counter to detect and

count fast particles.

The experiment was conducted, as is shown below. Alpha particles were

fired from a source (from within a lead "shield") at a sheet of thin

gold foil (which had been beaten to about 400 atoms thick. A

fluorescent screen was placed behind / around the gold foil. Every

time an Alpha particle hit the screen a flash of light, or

"scintillation" was produced. This was conducted inside a vacuum (To

minimize alpha loss by scattering from air molecules).

Most of the particles went straight through the foil without any

deflection - however some of the particles (about 1 in 8000) were

deflected by a degree of more than 90 degrees.

This meant that the idea of the "Plum pudding" model (suggested by

J.J. Thompson in 1906) was in dispute - a model which Rutherford

himself had been a believer in.

Rutherford pondered this problem for some months. He eventually

decided there was simply no way it could generate the strength of

electric field necessary to deflect the fast moving alphas.

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