In a cyclotron, we want to determine what the frequency of revolution of a charged particle in a magnetic field is independent of.
The cyclotron frequency (\(f\)) is the frequency at which a charged particle revolves in a uniform magnetic field. It's given by:
\(f = \frac{qB}{2\pi m}\)
Where:
From the formula, we can see that the frequency \(f\) depends on the charge \(q\), the magnetic field \(B\), and the mass \(m\). It does *not* directly depend on the energy of the particle. However, this is true only for non-relativistic speeds. At relativistic speeds, the mass of the particle increases with its energy, and thus the frequency does become energy-dependent. *For the standard introductory physics treatment of the cyclotron, however, we assume non-relativistic speeds*.
Assuming non-relativistic speeds, the frequency of revolution of the charged particle in a magnetic field in a cyclotron is independent of its energy.
In a cyclotron, the frequency \( f \) of a charged particle is given by the formula: \[ f = \frac{qB}{2\pi m} \] where:
\( q \) is the charge of the particle
\( B \) is the magnetic field strength
\( m \) is the mass of the particle
From this equation, we can see that the frequency depends on the charge \( q \), magnetic field \( B \), and mass \( m \), but it does not depend on the energy of the particle. This is because the energy influences the velocity of the particle, but the frequency of revolution remains unaffected by the speed (and hence the energy) of the particle. Thus, the frequency of revolution is independent of its energy.