||
时空可变系多线矢物理学的创建、作用与发展(29)引力也是辏力,
(接(28))
当引入辏力的相应表达式,设M(0(0))足够大,引力中心与参考系原点(0)相重,且运动仅限于在[基矢012] 3-维时空内 (即Newton 引力),并取变换:
1/L(0) =[r(1-0(0(3)))r=[r(1-0(0,b))^2,b=1到3求和]^(1/2),上式简化为:
[矢F引(1-0(0,0)]~- ict(1-0(0))KM(0(0))M(0(1)L(0)^3(1+((rp(12))/(M(0(1)c))^2
((dL(0)/d[角r(0,1)])^2+ L(0)^2))^2;
[矢F引(1-0(0,1)]~-KM(0(0))M(0(1)L(0)^
[矢F引(1-0(0,2)]~-KM(0(0))M(0(1)L(0)^2 s(r(0,1)) (1+((rp(12))/(M(0(1)c))^2 ((dL(0)/d[角r(0,1)])^2+ L(0)^2))^(1/2);
[矢F引(1-0(0,3)]=0, ((0):, (1) 均实物粒子)
[矢F引(1-0(0,0)]~- ict(1-0(0))KM(0(0))h[频率(1)]c^(-2)(rp(12))L(0)^3
((dL(0)/d[角r(0,1)])^2+ L(0)^2))^(1/2);
[矢F引(1-0(0,1)]~-KM(0(0))h[频率(1)]c^(-2)(rp(12))L(0)^
((dL(0)/d[角r(0,1)])^2+ L(0)^2))^(1/2);
[矢F引(1-0(0,2)]~-KM(0(0))M(0(1)h[频率(1)]c^(-2)(rp(12))L(0)^2 s(r(0,1))
((dL(0)/d[角r(0,1)])^2+ L(0)^2))^(1/2);
[矢F引(1-0(0,3)]=0, ((0):实物粒子, (1):光子) (8.5)
(未完待续)
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