Some Problems Raised by the Unified Field Theory
Marie Antoinette Tonnelat · 2014
V2 (C{JIIV P + C{JPIl v + C{Jz..I&s;P II) = 0, 21-", 2 &s; 2 ,I-" (7. 66) (7. 67) div 2C{Jpq = 0 p Tpq = 0, (7. 68) (7. 69) If we consider now an electric charge to be a singularity creating the field ~, we must introduce the potential To determine the equations of motion, we must use the equations 1 -e = (Rpq - Gpq) - - 4 pq 4 4 2 pq 4 SS 4 S (7. 73) - ( ~4 - G44 ) ] &s; 4 4 - 8pq = a r( Cpps a sc.o,qr + orp asq cpa SCP - opqors cp as cp) , 4 2 2 22 22 (7. 74) whence J 8pk nk ds = 41T Cp(k) 4 4 -~pq = or Fpqr, Fpqr = - Fprq &s; whence (7. 76) (7. 77) (7. 78)