(1) Solutian of interacting charged partscles System lagrongian Correct to rdeu the Lomplele daTurn utfen しinclusie be as Can ViVj Lrautn 2. 4 whee -1a-スj1, T Unit is a YP dinecion lagrangian en does not the correspen ding dapend erplterty The hamittantan on time, So - L energy of the Sstem. consewed the ViVi where + へ w ニ 2 c2 jei 2cij e canontcal mementum ef parhcle T fs he hanattaniarn Hence, he heravar
201j &c. as inst deived by dorusn But this s not Le af the formLL, FL Let the Lagrangian to dhe huncion L Carecion where s a then correspanding addition by H the hamittanian 1s se lated This sugests hat if we wish to exKpress he hami Hanian lerergy dhen ef and ntesms C.) .t) carrect inkerpretation A that mere -Ce) which indicades hat a funtdion the. hamitaniom f e dhe Coesdinales Coes pundine and he Canonical Corre ctian momanta P. So the Smat
be L to he lagrangtan hould expressed io befere subsdracting dems ofp and 4Re rom dAe lowest CYdear derm he hamil- could ecasd then, ene hamiltanian ef and -1anian enegy Tr eems teems ot Ce.1) aesult o destsed which can to ,) . e, Contributins louest esdes hami In the present example, the momenta, ot cancnical tanian Aeems Ho Vi 1,j 2 mi Canection dhe the to Smal desuibe FO lagrungian e Daruin dhe Pi, teams than the Sudtices to arpoxate adher the relatin (3) as oC) have Then ue C 2m;mj
rom uhich oblain the danwtn hamiltaniann we fi 2m; , j 2m,myCe hamiltanian to fist This is he arder charged of two Case particles Cm,a) now, fer dhe ond Lm,) Y =1,-, P, P P we get putir these 4 2t m m3 2m,