Can someone explain to me how work can be both a conservative force (which is indepedent of path) and a path function (which depends upon the pathway used to achieve any state)?
I'm not sure exactly what you mean, but
work is always path dependent!
BY DEFINITION: Work = F dot d or Fd cos(theta)
When one talks of work done against gravity for example: if you lift an object straight up at a constant velocity to height h. You have done work by imparting a force (mg) for a distance h....thereby giving you work done (mgh), which happens to equal the gain in graviational potential energy.
In the kinetic work energy theorem (assuming mass is constant): When kinetic energy is changed, a force (and hence acceleration (+ or -)) had to applied over a distance d in order to change the velocity. If this force happened to be gravity, so be it. It still does work along the F dot d or Fd cos (theta). F due to gravity just happens to always point straight down.
P delta V work is also path dependent. See heat engines for an example of this.
Regardless it is always path dependent.
EDIT: Now I understand your concern.....I think you are trying to differentiate between potential energies, which are functions of the potential energy fields (electric, gravitational etc.) from which they are derived and the work done by the force. Still work is always path dependent. The potential energies associated with an object/particle are more accurately correlated with their position in that particular energy field (gravitational, electro-magnetic). I'm sure you can consider them interchangable if you want to. But I choose not to take the chance of mis-cataloguing the energy changes. To each their own I suppose.