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A Thomson-type experiment with relativistic electrons. One of the earliest experiments to show that p=γm v (rather than p=m v ) was that of Neumann. [G. Neumann, A n n. Physik 45:529 (1914)]. The apparatus shown in Figure P4.5 is identical to Thomson's except that the source of high-speed electrons is a radioactive radium source and the magnetic field 𝐁 is arranged to act on the electron over its entire trajectory from source to detector. The combined electric and magnetic fields act as a veloc
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