The following is a derivation and motivation for the linearized DC-OPF. This discussion is adapted from (Broad. 19996).
r+jx | Impedance represented by the resistance respectively. |
G+jB | Real and imaginary terms of admittance (inverse of impedance). Note that the approximations of the imaginary term, 1/x is called susceptance. |
bus | Constant voltage construction to which transmission lines are connected. |
|V|q | Indicates voltage magnitude and phase angle at a system bus. |
p.u. | "per unit" indicates that the quantity has been scaled down for power calculations, where the scaling is specified by both a kilovolt and megawatt rating for any given section of the power system. |
The linearized DC load flow model is motivated by the observations that in large high voltage power systems:
Hence the following approximations can be made:
(Broad, 1996) shows that these assumptions lead to the equation for power flow on a line:
fkl = −Bkl(qk − ql) = gkl(qk − ql)
where gkl is the susceptance such that gkl = -Bkl = 1/ x
Thus the power flow equations are entirely linear and can be represented directly in a linear programming (LP) framework.
To formulate the OPF in PLEXOS, reactance is converted to susceptance using the formula:
gkl = 1/x
The susceptance determines the power flow on a line using the equation:
fkl = gkl (qk - ql)
In this equation qk - ql is the phase angle difference between the buses at each end of the line, measured in radians.