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相對論、量子力學及其場論的,本質、規律,及其必然且必需的發展(75)
引力也是輳力
(接(74))
當引入輳力的相應運算式,設M(0(0))足夠大,引力中心與參考系原點(0)相重,且運動僅限於在[基矢012] 3-維時空內 (即Newton 引力),並取變換:
1/L(0) =r(1-0)(3)=[r(1-0)(b))^2,b=1到3求和]^(1/2),上式簡化為:
[矢F引(1-0)0]~- ict(1-0)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)1]~-KM(0(0))M(0(1)L(0)^2 c(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)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)3]=0, ((0):, (1) 均實物粒子)
[矢F引(1-0)0]~- ict(1-0)KM(0(0))h[頻率(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)1]~-KM(0(0))h[頻率(1)]c^(-2)(rp(12))L(0)^2 c(r(0,1))
((dL(0)/d[角r(0,1)])^2+ L(0)^2))^(1/2);
[矢F引(1-0)2]~-KM(0(0))M(0(1)h[頻率(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)3]=0, ((0):實物粒子, (1):光子)
(未完待續)
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