What you are looking for is thus, "between what points in the Z direction is the bias applied", is that right?
That is an important question, of course. The simple answer is that the bias is applied from the left end of the left electrode to the right end of the right electrode.
Let us schematically draw a two-probe system as L-1|L|C|R|R+1, where L/R are the left/right electrodes (and L-1/R+1 are identical copies of them) and C the central scattering region. The reason we include L-1 and R+1 is because ATK assumes that atoms in L (R) may only interact with atoms in L-1 (R+1), and therefore from ATK's internal perspective, the complete system calculated is actually the one written above (from L-1 to R+1).
The Poisson equation is solved in the region L|C|R.
If periodic boundary conditions are used, ATK uses an FFT method, and the bias can be taken out of the equation since it is represented by a linear additive term to the potential, and the second derivative of that is zero. The boundary conditions are then such that the electrostatic potential at the left boundary of the left electrode match the bulk-like potential in L-1, and correspondingly for the right boundary of the right electrode. The bias is then added to the solution as a linear ramp.
If the system is heterogeneous, for example if the left and right electrodes have different spin or if they are geometrically different, a real-space finite difference multi-grid method is used, and the bias is explicitly included in the left and right boundaries as a rigid shift of the corresponding bulk-potentials from L-1 and R+1 on the edges.
Thus, the "voltage drop" occurs over the length of the two electrodes plus the central region, as illustrated in the plots in e.g.
this topic.