Dynamic co-simulation of start stop starter motor solenoid using Matlab & Edyson
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1 Dynamic co-simulation of start stop starter motor solenoid using Matlab & Edyson by Veerakumar G (RBEI/ENF8) Veerakumar.gopalan@in.bosch.com Associate Project Manager Robert Bosch Engineering and Business Solutions Private Limited
2 Agenda: 1. Start-Stop function overview 2. Starter Motor Basic components 3. Starter motor starting circuit 4. Solenoid mathematical model 5. Start-Stop solenoid functions 6. Problem statement 7. Approach used to solve the problem by co-simulation 8. Dynamic Interaction between Magnetic & System level domain 9. Robustness check for given variables 10.Results of co-simulation [Sample] 2
3 1. Overview : Start-Stop function Vehicle with manual transmission When the vehicle comes to a stop the engine is immediately switched off when the gear lever is in neutral and the clutch pedal is released Activating the clutch pedal once again restarts the engine automatically. Vehicle with automatic transmission After the brake pedal has been depressed, the engine is switched off as soon as the vehicle comes to a stop. When the brake pedal is released, the engine restartsrapidly and reliably Reduction of fuel & Co 2 up to 8% 3
4 2. Starter Motor Basic components 4
5 3. Starter Motor starting circuit General Starting circuit 5
6 Flux or Force Dynamic co-simulation of start stop starter motor solenoid using Matlab & Edyson 4. Solenoid mathematical model The solenoid behaviour is characterized by using Simscape language. It has electrical pins on left side which are input(p) and ground(n). It has input pin on right side which accepts magnetic flux. It has output pin which produces total ampere-turns (AT) depending up on the dynamic current. P N 6 Solenoid model Flux AT Flux data Force data Applied to mechanical system modelled in Simscape For different AT s Air gap The magnetic force and flux lookup tables need position and ampere turns as input in order to get relevant force and flux data for next simulation time steps.
7 5. Start Stop Solenoid functions Function Engage Only Pull the engage armature to the switching armature Keep the switch armature in rest position Energize only engage winding EA EA SA Engagement action Both the actions can be performed independently in order to fulfil the requirement of CoM [Change of Mind] conditions Function Switch Only Pull switch armature to the magnetic core Keep the engage armature in rest position Energize only switch winding SA Core Function key start 7 Engagement action should follow the switching action. Both the windings need to be energized appropriately. Switching action Core
8 6. Problem statement The look up table method holds good for single moving armature against stationary magnetic core. If there are two movable armatures the generation of force and flux data tables will become more complex since we do not have fixed reference frame for EA because SA can also move with in its design space. Similarly for SA we should also know the dynamic position of EA in-order to calculate the net magnetic force acting on SA. The complexities are 8 When engage winding is energized for engagement action, the switch armature dynamic position should be known. When switch winding is energized for switching action, the engage armature rest position should be known. During key start, engage windings will be energized first and with time delay switch winding will be energized, depending up on the positions of armatures and net magnetic force balance the armatures will move relatively and together towards fixed magnetic core.
9 7. Approach used to solve the problem Co-simulation is the efficient way to solve this problem Solenoid Model [EDYSON] only EMAG EA & SA Magnetic force for given dynamic positions of both the armatures The dynamic positions are calculated for applied magnetic force along with whole starter motor modelled in Simscape Solenoid Model-Mech., along with complete system [MATLAB/ Simscape] 9
10 8. Dynamic Interaction between Magnetic & System level domain Magnetic force generated depending up on the armature positions applied to mechanical systems Dynamic armature positions from Matlab for applied magnetic force 10
11 9. Robustness check Pinion to Ring gear distance Temperature Power net conditions Friction Magnetic force Spring force 11
12 10. Dynamic Co-Simulation Results Dynamic armature positions are shown for given boundary conditions Velocities shows the dynamic interaction between armatures 12
13 13
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