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By Gail Dyer.

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The ion is therefore further accelerated in the gap and enters D1. On account of its increased speed its semicircular path in D1 is of greater radius. The time of passage through D1, however, is still the same. , and the ion gains speed each time it passes from one dee to the other. Finally, the ion reaches the outer edge of one dee where it is pulled out of the system by a negatively-charged deflector plate. Evidently, eq. , is the resonance condition for the successful operation of the cyclotron.

They participate in weak interaction with matter. Quantum Physics 42 Mesons : These are middle-weight particles having masses intermediate between the muons and the nucleons (protons and neutrons). They are all bosons having zero spin and are unstable. They include pions (π+, π–, π°), kaons (K+, K–, K°, K ) and the eta-meson (η°). (i) Pi-mesons (or Pions) : Pi-mesons were discovered in 1947 in the upper atmosphere, although their existence was predicted much earlier by Yukawa in his meson theory of nuclear forces.

If v be the instantaneous speed of the electron, the instantaneous radial force on it will be Brev. This must be equal to the centripetal force mv2/r. Thus Brev = mv2 . r Therefore, the instantaneous momentum of the electron is p = mv = Brer. The rate of change of momentum is dp = dt d  b1 er  dBr = er . dt dt By Newton’s law this must be equal to a tangential force F acting on the electron. Thus F = er dBr . dt ... (iii) Quantum Physics 62 Clearly this force arises by the increasing flux density Br at the orbit.

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