Bohr静电荷模型(p132“Bohr理论") e圆周运动 +1 静电引力F= e =向心力F 4兀 07 nh 与1900 Plank 因此 my r m y I Bohr:2兀 n△E=mh 合称旧量子论 4E P 4TEnh =52917720837(pm)=ao ne 4mn e e ny 即 e 又∴ 48r 4兀cnr E=T+v mv+ 13.6 4丌6r)24兀6r4兀52×47627• Bohr静电荷模型 (p132 “Bohr理论”) : r mv F r e F 2 2 0 2 4 静电引力 = =向心力 =   e圆周运动 +1 e - m r P m r m v r r e m v r 2 2 2 2 2 2 0 2 4    因此 = = = n nh P = =   2 Bohr : 与1900 Plank  = nh 合称 旧量子论 0 2 2 2 2 2 0 2 2 0 52.91772083 (pm) 4 4 4 n a m e n h m e P r = = = =       r e mv r mv r e 0 2 2 2 2 0 2 4  4  又 = ，即 = E =T +V 2 0 2 0 2 0 2 0 2 2 1 13.6 2 4 4 2 4 1 2 4 1 r n e r e r e r e mv = −  =  − = −         = + −        