Power System Restoration With Transient Stability
Authors: Hassan Hijazi, Terrence W.K. Mak, Pascal Van Hentenryck
AAAI 2015 | Conference PDF | Archive PDF | Plain Text | LLM Run Details
| Reproducibility Variable | Result | LLM Response |
|---|---|---|
| Research Type | Experimental | Experimental results on existing benchmarks confirm the feasibility of the new approach. |
| Researcher Affiliation | Collaboration | Hassan Hijazi and Terrence W.K. Mak and Pascal Van Hentenryck NICTA and Australian National University 7 London Circuit, Canberra, ACT 2601, Australia {Hassan.Hijazi,Terrence.Mak,Pascal.Vanhentenryck}@nicta.com.au |
| Pseudocode | No | The paper includes mathematical models and a flow chart, but not structured pseudocode or algorithm blocks. |
| Open Source Code | No | The paper does not provide an explicit statement or link for open-source code for the methodology described. |
| Open Datasets | Yes | We have tested our model on 5 MATPOWER benchmarks (Zimmerman, Murillo-S andnchez, and Thomas 2011). |
| Dataset Splits | No | The paper uses standard MATPOWER benchmarks but does not specify any training/validation/test dataset splits, as it applies an optimization model rather than a machine learning training process requiring such splits. |
| Hardware Specification | No | The paper does not provide specific hardware details (e.g., CPU, GPU models, memory) used for running its experiments. |
| Software Dependencies | Yes | Our model is implemented in AMPL (Fourer, Gay, and Kernighan 2002; AMPL 2014), and uses Ipopt 3.11 (W achter and Biegler 2006) as a nonlinear solver. |
| Experiment Setup | Yes | Table 1 presents experimental results for various generator reactances and maximum rotor swing limits δ. The table presents aggregate results obtained by summing up all the objective values after solving Model 2 for all of the restoration steps (after filtering and simplification). Note that, in general, a rotor angle limit of 90 degrees is considered acceptable, the goal of the current experiment is to push the limits on this bound as far as possible. (T = 400, = 0.005) |