The ##IMG## [http://ej.iop.org/images/1063-7869/63/6/601/toc_tex_pu_8807_img1.gif] {$ k$} coefficient method proposed by Bondi is extended to the general case where the angle ##IMG## [http://ej.iop.org/images/1063-7869/63/6/601/tex_pu_8807_img2.gif] {$ \alpha$} between the velocity of a signal from a distant source at rest and the velocity of the observer does not coincide with 0 or ##IMG## [http://ej.iop.org/images/1063-7869/63/6/601/tex_pu_8807_img3.gif] {$ \pi$} , as considered by Bondi, but takes an arbitrary value in the interval ##IMG## [http://ej.iop.org/images/1063-7869/63/6/601/tex_pu_8807_img4.gif] {$ 0\le \alpha \le \pi$} , and to the opposite case where the source is moving and the observer is at rest, while the angle ##IMG## [http://ej.iop.org/images/1063-7869/63/6/601/tex_pu_8807_img2.gif] {$ \alpha$} between the source velocity and the direction ...

中文翻译：

---

## IMG ## [http://ej.iop.org/images/1063-7869/63/6/601/toc_tex_pu_8807_img1.gif] {$ k $}系数方法的广义相对论是观察者（光源）的速度和从（到）遥远光源（o ...

邦迪提出的## IMG ## [http://ej.iop.org/images/1063-7869/63/6/601/toc_tex_pu_8807_img1.gif] {$ k $}系数方法扩展到一般情况，来自遥远源的信号速度之间的角度## IMG ## [http://ej.iop.org/images/1063-7869/63/6/601/tex_pu_8807_img2.gif] {$ \ alpha $}静止并且观察者的速度与0或## IMG ##不重合[http://ej.iop.org/images/1063-7869/63/6/601/tex_pu_8807_img3.gif] {$ \ pi $}，由Bondi认为，但是在## IMG ##区间中采用任意值[http://ej.iop.org/images/1063-7869/63/6/601/tex_pu_8807_img4.gif] 0 \ le \ alpha \ le \ pi $}，相反的情况是源在移动，观察者处于静止状态，而角度## IMG ## [http://ej.iop.org/images/ 1063-7869 / 63/6/601 / tex_pu_8807_img2。gif]源速度和方向之间的{$ \ alpha $} ...