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时空可变系多线矢物理学的创建、作用与发展(27)
当[频率(1)] (偏分r(1-0(0,a) r(1-0(0,b)), b=0到3求和])=0;
[(dr(1-0(0,j)/dt(0))(偏分r(1-0(0,a)(dr(1-0(0,j)/dt(0)) ,a=0到3求和] =0,
(接(26))
简化为:
[矢F引(1-0(0)]
=-KM(0(0))M(0(1))(1-[r(1-0(0,j))时间导数^2/c^2,j=1到3求和] )^(-1/2)
([r(1-0(0,b ))^2, b=0到3求和] )^(-3/2)
[[r(1-0(0,b ))(偏分r(1-0(0,a) r(1-0(0,b)), b=0到3求和]
[基矢0(a)],a=0到3求和], ((0):实物粒子, (1):光子)
=-KM(0(0))h[频率(1)]c^(-2)[r(1-0(0,b))^2,b=0到3求和]^(-3/2)
[[r(1-0(0,b))(偏分r(1-0(0,a) r(1-0(0,b)), b=0到3求和])
[基矢0(a)],a=0到3求和], ((0):实物粒子, (1):光子) (8.3)
(未完待续)
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