Let's examine for a moment the mechanism thing. Consider a catenary cable and then we put it in a weightless environment. As soon that happens, the catenary becomes only ONE of the possible solutions to the directrix of the cable without any stiffness in a weightless environment: any path of the same length -even with kinks- is a solution to the cable position.
For a cable with some stiffness, a initial position, and a set of excitations and environment, the actual position can only then be derived from the laws of the mechanics. In absence of such data and process, every line of equal length is a solution.
What means:
That the solution -we are not to forget it is a solution got by SAP2000 v.15- of my entry 5 Aug 12:05 is but, if something, in spite of its apparent beauty, at most, just one of many possible solutions, because whatever the predominance of the tightening produced by the cables of the top of bottom set, the other has ample deformation ability to soak the required movement without problem; hence the sets of solutions really are all those that require the cinematics (as related to the measure of the cables with some holgure) of the problem. The "solution" found by SAP2000 must then, more than anything a device of its inner workings, since nothing really impels the outfit to the final shape shown in the image other than the relaxation worked by the program, and it is patent that there are many other positions that also satisfy the necessary requirements of relative positions between the parts after the descent of temperature.
Hence, for non-taut cables, the weightless environment becomes a severe requirement from the viewpoint of structural analysis since it widens the scope of the satisfactory solutions. A such cable is a mechanism able to take every shape compatible with its length, even with kinks (like chain links of the length of the elements, as, I remark, is the case, since the deformed shape shows such unnatural kinks ... because there is not a gravity forcing to take some catenary shape, or stiffness present to force some constant angle at a node.