For synchronous particles to remain on a constant radius in a synchrotron, show that the time derivative of the magnetic field is given by dB BATtum dt 2xqpR where ATturn is the kinetic energy gain per turn, R is the radius and p the bending radius, q the charge of a particle, ẞ=v/c. Assume the particles are accelerated on crest in a synchrotron of 10 GeV (kinetic energy) where the magnetic field reaches 1.5 Tesla in one second, following a linear variation. Calculate the bending radius and assuming R~1.5p, evaluate the accelerating voltage in kV.

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For synchronous particles to remain on a constant radius in a synchrotron, show that the
time derivative of the magnetic field is given by
dB
BATtum
dt 2xqpR
where ATturn is the kinetic energy gain per turn, R is the radius and p the bending
radius, q the charge of a particle, ẞ=v/c. Assume the particles are accelerated on
crest in a synchrotron of 10 GeV (kinetic energy) where the magnetic field reaches
1.5 Tesla in one second, following a linear variation. Calculate the bending radius
and assuming R~1.5p, evaluate the accelerating voltage in kV.
Transcribed Image Text:For synchronous particles to remain on a constant radius in a synchrotron, show that the time derivative of the magnetic field is given by dB BATtum dt 2xqpR where ATturn is the kinetic energy gain per turn, R is the radius and p the bending radius, q the charge of a particle, ẞ=v/c. Assume the particles are accelerated on crest in a synchrotron of 10 GeV (kinetic energy) where the magnetic field reaches 1.5 Tesla in one second, following a linear variation. Calculate the bending radius and assuming R~1.5p, evaluate the accelerating voltage in kV.
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