Chapter 11 - Magnetic Forces and Fields
Chapter 11.1 - Magnetism and Its Historical Discoveries
Chapter 11.2 - Magnetic Fields and Lines
Chapter 11.3 - Motion of a Charged Particle in a Magnetic Field
If a particle is moving in a direction perpendicular to a magnetic field, then the particle will take on a circular orbit.
Cyclotron Formulae
The centripetal force experienced by the particle, due to the magnetic field:
$$ F_B = q v B = \frac{m v^2}{r} $$
The radius of orbit that the particle will circle around:
$$ r = \frac{m v}{q B} $$
The period of motion for the particle in orbit:
$$ T = \frac{2 \pi r}{v} = \frac{2 \pi}{v} \frac{m v}{q B} = \frac{2 \pi m}{q B} $$
The maximum speed of a particle in a cyclotron:
$$ v_{max} = \frac{q B R}{m} $$
- $v_{max}$ the maximum speed
- $R$ the maximum orbital radius
The kinetic energy of a particle in a cyclotron:
$$ KE = \frac{1}{2} m v^2 = \frac{q^2 B^2 R^2}{2m} $$
The angular speed $\omega$ of a particle in orbit:
$$ \omega = \frac{v}{r} = \frac{q B}{m} $$
Helical Motion
The perpendicular component of helical motion, which causes the particle to orbit in a circular path:
$$ v_{perp} = v \ sin(\theta) $$
The parallel component of helical motion, which causes the particle to travel forward:
$$ v_{parallel} = v \ cos(\theta) $$
The pitch $p$ of the helix, the distance between adjacent turns
$$ p =v_{parallel} * T $$