Fulton and Rohrlich showed that this phenomenon is charge-independent when hyperbolic paths are considered, which may be a threat to the equivalence principle. Landau and Lifshitz's iterative treatment of this phenomenon eliminates the term for the Schott energy in an equation describing this phenomenon. Considering this phenomenon for a dumbbell-shaped distribution, then taking the limit of the size of the dumbbell to zero, underestimates its magnitude by 50%. The magnitude of this phenomenon in the original derivation is equal to mu sub naught times q squared over six pi c, all times the time derivative of the (*) acceleration. The original derivation of this pheno
Fulton and Rohrlich showed that this phenomenon is charge-independent when hyperbolic paths are considered, which may be a threat to the equivalence principle. Landau and Lifshitz's iterative treatment of this phenomenon eliminates the term for the Schott energy in an equation describing this phenomenon. Considering this phenomenon for a dumbbell-shaped distribution, then taking the limit of the size of the dumbbell to zero, underestimates its magnitude by 50%. The magnitude of this phenomenon in the original derivation is equal to mu sub naught times q squared over six pi c, all times the time derivative of the (*) acceleration. The original derivation of this phenomenon had acausal pre-acceleration solutions, in which the particle would respond to this phenomenon before it existed. For 10 points, name this phenomenon in which a particle's momentum is altered by the radiation it emits, first derived by Abraham and Lorentz.
Fulton and Rohrlich showed that this phenomenon is charge-independent when hyperbolic paths are considered, which may be a threat to the equivalence principle.
radiation reaction [or radiation recoil or self-force; accept Abraham-Lorentz-Dirac force before mention]