For a single charge at relativistic velocities, this quantity is proportional to the electron charge squared over the speed of light, times the Lorentz gamma raised to the sixth power. For a non-relativistic charge, this quantity is given by two-thirds times electron charge squared over speed of light cubed, times acceleration squared, a result called Larmor's formula. In electrodynamics this quantity is equal to the volume integral of current dotted with electric field; in that situation, this quantity is counterbalanced by a term that include
For a single charge at relativistic velocities, this quantity is proportional to the electron charge squared over the speed of light, times the Lorentz gamma raised to the sixth power. For a non-relativistic charge, this quantity is given by two-thirds times electron charge squared over speed of light cubed, times acceleration squared, a result called Larmor's formula. In electrodynamics this quantity is equal to the volume integral of current dotted with electric field; in that situation, this quantity is counterbalanced by a term that includes the divergence of the Poynting vector, which measures this quantity per unit area. In mechanical systems, this quantity is often given as the product of the force and the velocity. For 10 points, identify this quantity which gives the energy dissipated per unit time and is usually measured in Watts.
For a single charge at relativistic velocities, this quantity is proportional to the electron charge squared over the speed of light, times the Lorentz gamma raised to the sixth power.