时空可变系多线矢世界分享 http://blog.sciencenet.cn/u/可变系时空多线矢主人 演绎矢算研究高速运动且有相互作用的问题所不可缺少!

博文

一切物体的基本特性和运动规律 (11)

已有 424 次阅读 2019-8-14 12:51 |个人分类:物理|系统分类:论文交流

一切物体的基本特性和运动规律 (11)

    ((10))

八.由可变系时空多线矢,分析强力、弱力的基本特性

强力与弱力都是时空12维的22,1线矢

强力与弱力(一切粒子都有相应的质量、动量、强自旋,因而,也都有相应于强自旋的强力与弱力)

32. (偏分(4)v(4))(6)[2线矢]

偏分(4)v(4))(6)[2线矢]=偏分(4) [1线矢]叉乘v(4)) [1线矢]

  ={(v(4)j/r(4)0-v(4)0/r(4)j) [基矢0j]

+(v(4)l/r(4)k-v(4)k/r(4)l) [基矢kl],jkl=123循环求和}

各粒子的强自旋:

33. 强自旋S(15)[22线矢]

=(偏分(4)v(4))(6)[2线矢]叉乘自旋S(6)[2线矢]

={(v(4)j/r(4)0-v(4)0/r(4)j) [基矢0j]

+(v(4)l/r(4)k-v(4)k/r(4)l) [基矢kl],jkl=123循环求和}叉乘

{(p(4)j/r(4)0-v(4)0/r(4)j) [基矢0j]

+(p(4)l/r(4)k-p(4)k/r(4)l)[基矢kl],jkl=123循环求和},

{注意:p(4)=m0 v(4)/(1-(v(3)/(c(光传)a*(声传))^2)^(1/2)

并令:[]=(1-(v(3)/(c(光传)a*(声传))^2)^(1/2)

= m0{[(v(4)k/r(4)0-v(4)0/r(4)k)

((v(4)l/[])/r(4)0-(v(4)0/[])/r(4)l)

-(v(4)l/r(4)0-v(4)0/r(4)l)

((v(4)k/[])/r(4)0-(v(4)0/[])/r(4)k)][基矢0k,0l]

+[(v(4)l/r(4)k-v(4)k/r(4)l)

((v(4)j/[])/r(4)l-(v(4)l/[])/r(4)j)

-(v(4)j/r(4)l-r(4)l/r(4)j)

((v(4)l/[])/r(4)k-(v(4)k/[])/r(4)l)][基矢kl,lj]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((v(4)l/[])/r(4)k-(v(4)k/[])/r(4)l)

-(v(4)l/r(4)k-v(4)k/r(4)l)

((v(4)j/[])/r(4)0-(v(4)0/[])/r(4)j)][基矢0j,kl]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((v(4)j/[])/r(4)l-(v(4)l/[])/r(4)j)

-(v(4)j/r(4)l-v(4)l/r(4)j)

((v(4)j/[])/r(4)0-(v(4)0/[])/r(4)j)][基矢0j,lj]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((v(4)k/[])/r(4)j-(v(4)j/[])/r(4)k)

-(v(4)k/r(4)j-v(4)j/r(4)k)

((v(4)j/[])/r(4)0-(v(4)0/[])/r(4)j)][基矢0j,jk]

,jkl=123循环求和}

34. 强自旋光(15)[22线矢]

= {[(v(4)k/r(4)0-v(4)0/r(4)k)

((h光频率/c)l/r(4)0-(h光频率/c)0/r(4)l)

-(v(4)l/r(4)0-v(4)0/r(4)l)

((h光频率/c)k/r(4)0-(h光频率/c)0/r(4)k)][基矢0k,0l]

+[(v(4)l/r(4)k-v(4)k/r(4)l)

((h光频率/c)j/r(4)l-(h光频率/c)l/r(4)j)

-(v(4)j/r(4)l-r(4)l/r(4)j)

((h光频率/c)l/r(4)k-(h光频率/c)k/r(4)l)][基矢kl,lj]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((h光频率/c)l/r(4)k-(h光频率/c)k/r(4)l)

-(v(4)l/r(4)k-v(4)k/r(4)l)

((h光频率/c)j/r(4)0-(h光频率/c)0/r(4)j)][基矢0j,kl]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((h光频率/c)j/r(4)l-(h光频率/c)l/r(4)j)

-(v(4)j/r(4)l-v(4)l/r(4)j)

((h光频率/c)j/r(4)0-(h光频率/c)0/r(4)j)][基矢0j,lj]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((h光频率/c)k/r(4)j-(h光频率/c)j/r(4)k)

-(v(4)k/r(4)j-v(4)j/r(4)k)

((h光频率/c)j/r(4)0-(h光频率/c)0/r(4)j)][基矢0j,jk]

,jkl=123循环求和}

35. 强自旋声(15)[22线矢]

= {[(v(4)k/r(4)0-v(4)0/r(4)k)

((h声频率/a*)l/r(4)0-(h声频率/a*)0/r(4)l)

-(v(4)l/r(4)0-v(4)0/r(4)l)

((h声频率/a*)k/r(4)0-(h声频率/a*)0/r(4)k)][基矢0k,0l]

+[(v(4)l/r(4)k-v(4)k/r(4)l)

((h声频率/a*)j/r(4)l-(h声频率/a*)l/r(4)j)

-(v(4)j/r(4)l-r(4)l/r(4)j)

((h声频率/a*)l/r(4)k-(h声频率/a*)k/r(4)l)][基矢kl,lj]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((h声频率/a*)l/r(4)k-(h声频率/a*)k/r(4)l)

-(v(4)l/r(4)k-v(4)k/r(4)l)

((h声频率/a*)j/r(4)0-(h声频率/a*)0/r(4)j)][基矢0j,kl]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((h声频率/a*)j/r(4)l-(h声频率/a*)l/r(4)j)

-(v(4)j/r(4)l-v(4)l/r(4)j)

((h声频率/a*)j/r(4)0-(h声频率/a*)0/r(4)j)][基矢0j,lj]

+[(v(4)j/r(4)0-v(4)0/r(4)j)

((h声频率/a*)k/r(4)j-(h声频率/a*)j/r(4)k)

-(v(4)k/r(4)j-v(4)j/r(4)k)

((h声频率/a*)j/r(4)0-(h声频率/a*)0/r(4)j)][基矢0j,jk]

,jkl=123循环求和}

量纲:[M][T]^(-2)

     (未完待续)




http://blog.sciencenet.cn/blog-226-1193592.html

上一篇:坚决纠正:对“量子纠缠”、“量子计算机”、“单光子源”等基本观点的国际流行严重错误
下一篇:一切物体的基本特性和运动规律 (12)

0

该博文允许注册用户评论 请点击登录 评论 (0 个评论)

数据加载中...

Archiver|手机版|科学网 ( 京ICP备14006957 )

GMT+8, 2019-9-18 17:22

Powered by ScienceNet.cn

Copyright © 2007- 中国科学报社

返回顶部