Absolution of Energy by Electrons. 75 



to trace at t , and from t Q to t h it has been completely domi- 

 nated by the internal forces of the field. 



On solving the six equations for which (16) stands, 



»=6M f dx 



n=6 M ' C* dx 



*=1 AJt n C K 



A = 



rfp d<7 <#r rf# rfy ^ 



d/c 1 d/€ 1 d/c 1 d/Ci diCi d/Ci 



dic 2 



dp 



dtc 3 



dp 



d/c± 



dp 



d/c 5 



dp 



dtc 6 



M n = (M ln , M 2n , MJ 



(17) 

 (18) 

 (19) 



(20) 



M/ = {M w M 5n , MJ (21) 



Here M ln is the minor of the first column and nth row in 

 A, and the other symbols in (20) and (21) have like mean- 

 ings. It is well known that A is a constant independent of 

 the time, and if the constants k are the positions and 

 momenta at any one time A = l« 



The radiation is defined by the electromagnetic equations : 



I ^ = Curl H (22) 



c dt K J 



ldR 



c dt 



= -CurlE. 



E' = E+-[uH] 



(23) 

 (24) 



