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AN3327 Datasheet(PDF) 7 Page - STMicroelectronics

Part # AN3327
Description  L9942 back EMF stall detection algorithm
PDF  22 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

AN3327 Datasheet(HTML) 7 Page - STMicroelectronics

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AN3327
Universal motor concepts
19
2
Universal motor concepts
Motor voltage can be expressed in an equation consisting of three components, Resistive,
Electro-motive, and Inductive.
Equation 1
The Resistive component (RWindings) plays a big part in determining what stall current to
expect. When the motor is not spinning the only thing limiting the current is the winding
resistance.
The inductance of a motor (LWindings) is taken advantage of when PWM signal is applied.
The inductance allows for a constant or smooth phase current when the PWM frequency is
set such that the inductance supports the current in the windings during the PWM off-time.
The BEMF is the voltage that is generated by the motor as the permanent magnet armature
spins inside (or around) the stator. As the rotor spins the windings experience a changing
magnetic field. This changing magnetic field generates the BEMF voltage that is directly
related to the speed of the changing field.
There are two universal concepts in motors that are always true The first is that BEMF is
directly proportional to armature speed and really, nothing else. The back EMF equations
spell this out quite clearly:
Equation 2
Where:
•
N is the number of coil turns
•
B represents the magnetic field
•
A the area encompassed by the motor magnetic field
•ω is the angular speed
Notice that N, B, and A are all constants specific to the motor construction. They do not
change. The end result is that Back EMF (emf) is directly proportional to motor speed (
ωt).
The next universal concept is the relationship between motor torque and motor current.
Again, the equations describe this clearly:
Equation 3
V
Motor
i
Motor
R
Windings
BEMF
L
Windings
di
Motor
dt
-----------------
++
⋅
=
bemf
N
–
BA
ωωt
()
sin
⋅⋅ ⋅ ⋅
=
T
pN
2
π
--------
θI
=



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