Hmm... I still don't think so. What about if you have body forces? Then the internal stresses balance both the externally applied loads plus the volume forces. Do you agree with this? However, one can of course compute the internal stress plus the body force loading...
But then consider a cube with a non-uniform pressure on more than one side. How do I compute from this global vector the average or total load applied to any individual surface? You can't, because the values in the degrees-of-freedom shared by any two sides of the geometry contain load contributions from two faces. For reaction forces at constrained surfaces - no problem of course!
Also, I think that one should consider which vectors one typically constructs during assembly. The most efficient way to do assembly (but I recognise that this is not universally followed - not even by me) is to compute the constrained RHS vector and tangent matrix in one shot during assembly. That means that you never need to actually construct the individual internal, external and body force vectors in order to solve your linear system because, well, they get bundled into the RHS and then further manipulated when imposing constraints.
Dependent on what it is you want to achieve, I do concur that what you suggest may be perfectly plausible. But in general... I'm still unconvinced. To be introspective, what I suggest (and what Hamed has done here) might be overkill for plain elasticity alone since you can always recompute the traction vector itself as it is you that specified the loading at each time-/load-step. In coupled problems, however, external tractions are not always so easily defined and its actually sometimes easier to simply do this stress-type integration procedure.