The total power radiated is found by integrating this quantity over all solid angles (that is, over θ θ and ϕ ϕ ). This gives P = 2 3 q 2 a 2 c 3 , which is the Larmor result for a nonrelativistic accelerated charge. It relates the power radiated by the particle to its acceleration. It clearly shows that the faster the charge accelerates the greater the radiation will be. We would expect this since the radiation field is dependent upon acceleration.