Electrical and Electronic Engineering
p-ISSN: 2162-9455 e-ISSN: 2162-8459
2011; 1(1): 1-6
doi: 10.5923/j.eee.20111001.01
Ya-Chin Chang
Department of Electrical Engineering, Cheng Shiu University, No. 840, Chengcing Rd., Niaosong Dist., Kaohsiung City, Taiwan
Correspondence to: Ya-Chin Chang , Department of Electrical Engineering, Cheng Shiu University, No. 840, Chengcing Rd., Niaosong Dist., Kaohsiung City, Taiwan.
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Copyright © 2012 Scientific & Academic Publishing. All Rights Reserved.
In order to enable power systems to accommodate more power transfers with less network expansion by building new transmission lines, reinforcement of existing transmission networks is becoming more urgent. Installation of Flexible AC Transmission Systems (FACTS) devices can be a better choice among previous methods. The aim of the optimal shunt voltage compensator (SVC) installation problem proposed in the paper is to maximize the benefit from the future fuel expense with proper SVC installations such that transmission system loadability can be improved the most. A particle swarm optimization (PSO) algorithm involving in the continuation power flow (CPF) process is used to determine the optimal SVC installation for the network reinforcement. The effectiveness of the proposed solution method is validated with the SVC installations conforming to the benefit from the investment.
Keywords: Continuation Power Flow, FACTS, Particle Swarm Optimization, System Loadability, Tangent Vector
Cite this paper: Ya-Chin Chang , "Benefit-Based Optimal SVC Installation for Transmission System Loadability Enhancement", Electrical and Electronic Engineering, Vol. 1 No. 1, 2011, pp. 1-6. doi: 10.5923/j.eee.20111001.01.
![]() | (1) |
that, associated with a loading level, would drive the system from one stable equilibrium point to another, is inserted into the power flow equations, the system equations become: ![]() | (2) |
![]() | (3) |
![]() | (4) |
and
are the real and reactive power flows on bus i of line i-j;
and
are the base-case injections (including generation and load) to bus i;
,
and
are a set of specific loading increments related to the expected future increases of generation real power, load real and reactive powers on bus i,
,
denoting the set of the buses associated with the loading increments. If increases are not allowed,
,
and/or
would be zero. For clarity, the loading increments is denoted by a vector
and
defined as a loading increment path to make loadability increase, whereas
is used to seek for loadability along the loading increment path. The loadability =
, where
being the maximum value of
, as represents the critical value of a saddle-node bifurcation point for the system about to become instable. The
can also be referred to as the maximum LM or static voltage stability margin (VSM) for a specific loading increment, based on bus voltage stability collapse or critical constraints [16]. As an SVC installed on bus i, the reactive power balance equation can be expressed as: ![]() | (5) |
is the reactive power provided by the SVC installation. It is another decision variable that may lead the system to a new state, whose value should be within the limited ranges defined as:![]() | (6) |
is the set of the PQ buses specified for SVC installation.
and a unit change of parameter
, say
, expressed as: ![]() | (7) |
. If the functional vector
is used to denote the whole set of equations, the problem can be expressed by: ![]() | (8) |
, the base-case state
can be obtained first by using a conventional power flow method, and then
will be sought along the loading increment path by applying the CPF process. During the process, when no more increases, namely reaching
, eventually the loadability,
, is derived. CPF uses a predictor-corrector scheme along the loading increment path to find subsequent values of
. While the corrector is only a slightly modified Newton-Raphson power flow, predictor is quite unique from anything found in a conventional power flow and deserves detailed attention [16]. PredictorAfter the base-case state obtained, a prediction of the next solution can be made by taking an appropriately sized step in a direction tangent to the solution path (loading increment path). Thus, the first task in the predictor process is to calculate the tangent vector. This tangent calculation is derived by first making derivative to both sides of (8) as follows: ![]() | (9) |
that is directly associated with the base loading increment. In order to find a unique solution, an important barrier must be overcome. This problem arises when variable
was inserted into the power flow equations but the number of equations remains unchanged. Thus, one more equation is required. This problem can be solved by choosing a non-zero magnitude, say 1, from one of the components in the tangent vector. Since the equations in (9) are linear, let
be equal to 1 to simply denote the tangent vector and suppose
would increase in each step until
reached. Equation (9) is then augmented and becomes: ![]() | (10) |
is an appropriately dimensioned row vector with all elements equal to zero except the (
)th, which is equal to 1 associated with the unit change of
.Once the tangent vector is obtained by solving (10), the predication can be made by: ![]() | (11) |
and the scaling factor
should be appropriately chosen during each predication so that the solution can be within the convergence radius of the corrector.The corrector process is used to modify the predicted solution onto the solution path with one of the state variables being ascertained into an additive equation, say
. Then, the new set of equations would be: ![]() | (12) |
, assuming on bus k, which has the most negative value in the prediction. With an additive equation and variable
, the augmented equations can be solved by a slightly modified Newton-Raphson power flow method. For dealing with the saddle-node bifurcation point on the loading increment path, the CPFLOW method in [19] is employed to execute the CPF process. In this paper, by taking into account both technical and economical concerns, the maximum benefit from the investment for SVC allocation and the corresponding loadbility along the loading increment path will be solved with the following method.
[17]. The benefit rate from future system loadability is evaluated by: ![]() | (13) |
![]() | (14) |
(Mvar) is the capacity of the SVC installation at bus i. The unit of
is US$/Mvar.Obviously, the cost function in (14) must be unified into US$/MvarHr. Assume five years of its lifetime is employed, and the cost function for investment recovery becomes: ![]() | (15) |
; if
, set
to 1.0 p.u..The total cost to recover from the investment to the SVC installations is evaluated by: ![]() | (16) |
![]() | (17) |
![]() | (8) |
![]() | (19) |
![]() | (20) |
are sought via the CPF procedure along the loading increment path. The buses voltages are found when a terminated condition met. ![]() | Figure 1. Modified IEEE-14 bus system. |
|
|
, for the four cases are shown in Fig. 2. As seen that the maximum loadability (
) is obtained from case 1 and the most critical voltage magnitude found on bus 9 is equal to 8.20 p.u., which is the biggest in the four cases. Consequently, case 1 is chosen and the four buses 6, 9, 10 and 11 are specified for SVC installation. And then, the proposed method is used to solve for an optimal SVC installation based on the locations of case 1 specified for SVC installation.
|
![]() | Figure 2. P-V curves for the four cases. |
![]() | Figure 3. Course for Seeking maximum benefit rate and loadability. |
) using the proposed method is shown in Fig. 3. As can be found that the maximum benefit rate derived is 2414 (US$/Hr) and the corresponding loadability equals
=
, with the reactive powers provided by the four SVC installations being 1.398, 2.0, 1.745 and 0.502 p.u., respectively. In addition, it can also be found from Fig. 3 that, at 11th iteration, the reactive powers provided by the four SVC installations are 1.480, 2.0, 1.877 and 0.601 p.u. respectively, and the corresponding loadability equal to
= 4.08 p.u. is bigger than 4.035 p.u.. Therefore, it is found that a bigger loadability can be derived from a different SVC installation. With the same reactive powers provided by the SVC installations and only using
as the objective function to be maximized, the loadability is found to be 4.458 p.u., which is bigger than the others obtained before. The most critical voltage magnitude equal to 0.84 p.u. is found at bus 4. The capacities of the four SVC installations are set to 1.678 p.u., 2.40 p.u., 2.094 p.u. and 1.0 p.u., respectively. On the other hand, when network structure remains unchanged, namely without SVC installation, the loadability is found to be 3.715 p.u., as is much less than 4.458 p.u., and thus the effectiveness of the proposed SVC installation method is validated through the test.