Starter
Starter as a DC motor
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      Powertrain Blockset / 
      Energy Storage and Auxiliary Drive / 
      Starter
   
Description
The Starter block implements a starter assembly as a separately excited DC motor, permanent magnet DC motor, or series connection DC motor. The motor operates as a torque source to an internal combustion engine.
Use the Starter block:
- In an engine model with a front-end accessory drive (FEAD) 
- To model engine start and stop scenarios 
The Starter block supports only an angular speed input to the DC motor. A load torque input requires engine dynamics.
Separately Excited DC Motor
In a separately excited DC motor, the field winding is connected to a separate source of DC power.
The relationship between the field winding voltage, field resistance, and field inductance is given by:
The counter-electromotive force is a product of the field resistance, mutual inductance, and motor shaft angular speed:
The armature voltage is given by:
The starter motor current load is the sum of the field winding current and armature winding current:
The starter motor shaft torque is the product of the armature current, field current, and mutual inductance:
Permanent Magnet DC Motor
In a permanent magnet DC motor, the magnets establish the excitation flux, so there is no field current.
The counter-electromotive force is proportional to the motor shaft angular speed:
The armature voltage is given by:
The starter motor current load is equal to the armature winding current:
The starter motor shaft torque is proportional to the armature winding current:
Series Excited DC Motor
A series excited DC motor connects the armature and field windings in series with a common DC power source.
The counter-electromotive force is a product of the field and armature initial series current, field, and armature mutual inductance and motor shaft angular speed:
The field and armature winding voltage is given by:
The starter motor current load is equal to the field and armature series current:
The starter motor shaft torque is the product of the squared field and armature series current and the field and armature mutual inductance:
For motor stability, the motor shaft angular speed must be greater than the ratio of the series connected field and armature resistance to the mutual inductance:
Power Accounting
For the power accounting, the block implements these equations.
| Bus Signal | Description | Variable | Equations | ||
|---|---|---|---|---|---|
| 
 | 
 
 
 | 
 | Mechanical power | Pmot | |
| PwrBus | Electrical power | Pbus | Separately excited DC motor | ||
| PM excited DC motor | |||||
| Series excited DC motor | |||||
| 
 
 
 | PwrLoss | Motor losses | Ploss | ||
| 
 
 
 | PwrInd | Electrical inductance | Pind | Separately excited DC motor | |
| PM excited DC motor | |||||
| Series excited DC motor | |||||
The equations use these variables.
| Ra | Armature winding resistance | 
| La | Armature winding inductance | 
| EMF | Counter-electromotive force | 
| Rf | Field winding resistance | 
| Lf | Field winding inductance | 
| Laf | Field and armature mutual inductance | 
| ia | Armature winding current | 
| if | Field winding current | 
| Kt | Motor torque constant | 
| ω | Motor shaft angular speed | 
| Va | Armature winding voltage | 
| Vf | Field winding voltage | 
| Vaf | Field and armature winding voltage | 
| iaf | Field and armature series current | 
| Rser | Series connected field and armature resistance | 
| Lser | Series connected field and armature inductance | 
| iload | Starter motor current load | 
| Tmech | Starter motor shaft torque | 
Examples
Ports
Inputs
Output
Parameters
References
[1] Krause, P. C. Analysis of Electric Machinery. New York: McGraw-Hill, 1994.
Extended Capabilities
Version History
Introduced in R2017a

