I may be going off a little on a tangent, but this is the way it makes sense to be.
The load flow equations are the first equation here:
As it turns out, the off-diagonal elements of J and J^-1 are very close to zero for typical series transmission elements which are primarily inductive.
That is the basis for "decoupling" the real and reactive power equations during "fast decoupled load flow" method and also very useful for quick back-of-the-envelope qualitative analysis as we are discussing.
When real and reactive power are decoupled, real power flow through a series inductive element is dependent upon (or controls, depending on your viewpoint) the voltage PHASE angle difference accross that element (and is independent of the voltage magnitude difference accross that element). More importantly, reactive power flow through a series inductive element is dependent upon (or controls, depending on your viewpoint) the voltage MAGNITUDE difference accross that element (and is independent of voltage phase angle difference).
So again the last sentence is the important one. Vars control voltage magnitude. If there is a net vars flowing out of a node where caps are added, then that node will be higher voltage than whatever node those vars flow to. By mapping out the var flow in the system you can get a pretty good idea of the voltage distribution.
Sorry, if it's not what you're looking for.
=====================================
Eng-tips forums: The best place on the web for engineering discussions.