In an effort to minimize energy losses through the optimal control of an electric rapid transit system, three vehicle/flywheel configurations are modeled using the bond graph technique. Field and armature control of an on-board flywheel are presented along with field control of a station flywheel used in conjunction with a typical regenerative vehicle. Pontryagin's Minimum Principle is used to develop the optimal control trajectories for vehicle accelerations and decelerations. The time integral of mechanical and electrical losses is minimized as the cost function. Armature control of the hybrid vehicle and field control of the station flywheel are equally efficient in the reversible energy flow between vehicle and flywheel. Field control of the hybrid vehicle is slightly less efficient. The optimal trajectory for deceleration is nearly linear, but the optimal trajectory for acceleration, due to the effect of mechanical losses over a longer time period, is highly concave and differs radically from a typical transit acceleration. The vehicle weight and resistance in the armature windings have a large influence on system performance. (Author)
The Application of Optimal Control Theory to Hybrid Electric Transit Systems
1977
138 pages
Report
No indication
English
Metropolitan Rail Transportation , Miscellaneous Energy Conversion & Storage , Ground vehicles , Transportation , Flywheels , Energy storage , Efficiency , Armatures , Stators , Electrical resistance , Transit systems , Electric transit systems , Rapid transit systems , Hybrid vehicles , Control theory , Theses
The application of optimal control theory to hybrid electric transit systems
Tema Archive | 1977
|SAE Technical Papers | 1997
|Tema Archive | 1998
|Automotive engineering | 1998
|NTIS | 1997
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