Difference between revisions of "Synchrotron"
Jump to navigation
Jump to search
m (cat) |
m (links) |
||
| Line 1: | Line 1: | ||
| − | A synchrotron is a type of particle accelerator used to generate high intensity short wavelength (generally x-ray) radiation. | + | A '''synchrotron''' is a type of [[particle]] accelerator used to generate high intensity short [[wavelength]] (generally [[x-ray]]) [[radiation]]. |
A synchrotron consists of a linear accelerator which accelerates and channels electrons into a circular accelerator called a booster ring. In the booster ring the electrons are accelerated up to near relativistic velocities. They are they transferred to a storage ring where they are keept at a constant speed. As the electron goes around the storage its velocity changes and so it emits Bremsstrahlung (braking) radiation at a tangent to the loop. This radiation is much more intense than that generated by other methods at the same wavelength and has a large number of scientific applications. | A synchrotron consists of a linear accelerator which accelerates and channels electrons into a circular accelerator called a booster ring. In the booster ring the electrons are accelerated up to near relativistic velocities. They are they transferred to a storage ring where they are keept at a constant speed. As the electron goes around the storage its velocity changes and so it emits Bremsstrahlung (braking) radiation at a tangent to the loop. This radiation is much more intense than that generated by other methods at the same wavelength and has a large number of scientific applications. | ||
Revision as of 04:13, November 26, 2008
A synchrotron is a type of particle accelerator used to generate high intensity short wavelength (generally x-ray) radiation.
A synchrotron consists of a linear accelerator which accelerates and channels electrons into a circular accelerator called a booster ring. In the booster ring the electrons are accelerated up to near relativistic velocities. They are they transferred to a storage ring where they are keept at a constant speed. As the electron goes around the storage its velocity changes and so it emits Bremsstrahlung (braking) radiation at a tangent to the loop. This radiation is much more intense than that generated by other methods at the same wavelength and has a large number of scientific applications.