Motor constants

The constants K_M (motor size constant) and K_v (motor velocity constant, or the back EMF constant) are values used to describe characteristics of electrical motors.

Motor constant

K_M is the motor constant^[1] (sometimes, motor size constant). In SI units, the motor constant is expressed in (N⋅m/sqrt(W)):

K_{\mathrm {M} }={\frac {\tau }{\sqrt {P}}}

where

$\scriptstyle \tau$ is the motor torque (SI units, N·m)
$\scriptstyle P$ is the resistive power loss (SI units, W)

The motor constant is winding independent (as long as the same conductive material used for wires); e.g., winding a motor with 6 turns with 2 parallel wires instead of 12 turns single wire will double the velocity constant, K_v, but K_M remains unchanged. K_M can be used for selecting the size of a motor to use in an application. K_v can be used for selecting the winding to use in the motor.

Since the torque $\scriptstyle \tau$ is current I multiplied by K_T then K_m becomes

$K_{M}={\frac {K_{T}\cdot I}{\sqrt {P}}}={\frac {K_{T}\cdot I}{\sqrt {I^{2}\cdot R}}}={\frac {K_{T}}{\sqrt {R}}}$

where

$\scriptstyle I$ is the current (SI units, A)
$\scriptstyle R$ is the resistance (SI units, Ohm)
$\scriptstyle K_{T}$ is the Motor Torque Constant (SI units, N·m/A), see below

If two motors with the same K_v and torque work in tandem, with rigidly connected shafts, the K_v of the system is still the same assuming a parallel electrical connection. The K_M of the combined system increased by ${\sqrt {2}}$ , because both the torque and the losses double. Alternatively, the system could run at the same torque as before, with torque and current split equally across the two motors, which halves the resistive losses.

Motor velocity constant, back EMF constant

K_v is the motor velocity constant (not to be confused with kV, the abbreviation for kilovolt), measured in RPM per volt or radians per volt-second (rad/V-s):^[2] $K_{\mathrm {v} }={\frac {\omega _{\mathrm {No-Load} }}{V_{\mathrm {Peak} }}}$

The K_v rating of a brushless motor is the ratio of the motor's unloaded rotational speed (measured in RPM) to the peak (not RMS) voltage on the wires connected to the coils (the back EMF). For example, an unloaded motor of K_v 5,700 rpm/V supplied with 11.1 V will run at a nominal speed of 63,270 rpm (5,700 rpm/V × 11.1 V).

Actually, the motor may not reach this theoretical speed because there are non-linear mechanical losses. On the other hand, if the motor is driven as a generator, the no-load voltage between terminals is perfectly proportional to the RPM and true to the K_v of the motor/generator.

The terms K_e,^[3] K_b are also used,^[4] as are the terms back EMF constant.^[5]^[6] or the generic electrical constant.^[3] In contrast to K_V the value K_e is often expressed in SI units ${\frac {V\cdot s}{rad}}$ , thus it is an inverse measure of K_V.^[7] Sometimes it is expressed in non SI units V/krpm.^[8]

The field flux may also be integrated into the formula:^[9]

E_{b}=K_{\omega }\phi \omega

where

E_{b}

is back EMF,

K_{\omega }

is the constant,

\phi

is the flux, and

\omega

is the angular speed

An inverse measure is also sometimes used, which may be referred to as the speed constant.^[3]

By Lenz's law, a running motor generates a back-EMF proportional to the speed. Once the motor's rotational velocity is such that the back-EMF is equal to the battery voltage (also called DC line voltage), the motor reaches its limit speed.

Motor Torque constant

K_T is the torque produced divided by armature current.^[10] It can be calculated from the motor velocity constant K_v.

K_{\mathrm {T} }={\frac {\tau }{I_{A}}}={\frac {60}{2\pi \cdot K_{V}}}

where $I_{A}$ is the armature current of the machine (SI units A). K_T is primarily used to calculate the armature current for a given torque demand:

{I_{A}}={\frac {\tau }{K_{\mathrm {T} }}}

The SI units for the torque constant are newton-metres per ampere (N·m/A). Since N·m = J, and A = C/s, then N·m/A = J·s/C = V·s (same units as back EMF constant).

The relationship between K_t and K_v is not intuitive, to the point that many people simply assert that torque and K_v are not related at all. An analogy with an hypothetical linear motor can help to convince that it is true. Suppose that a linear motor has a K_v of 2 m/s per volt, that is, the linear actuator generates one volt of back-EMF when moved (or driven) at a rate of 2 m/s. Conversely, s=V·K_v (s is speed of the linear motor, V is voltage).

The useful power of this linear motor is P=V·I, P being the power, V the useful voltage (applied voltage minus back-EMF voltage), and I the current. But, since power is also equal to force multiplied by speed, the force F of the linear motor is F=P/(V·K_v) or F=I/K_v. The inverse relationship between force-per-amp and K_v of a linear motor has been demonstrated.

To translate this model to a rotating motor, one can simply attribute an arbitrary diameter to the motor armature e.g. 2 meters and assume for simplicity that all force is applied at the outer perimeter of the rotor, giving 1 meter of leverage.

Now, supposing that K_v (angular speed per volt) of the motor is 3600, it can be translated to "linear" by multiplying by 2π meters (the perimeter of the rotor) and dividing by 60, since angular speed is per minute. This is about 377 K_v linear (m/s per volt).

Now, if this motor is fed with current of 2 A and assuming that back-EMF is exactly 2 V, it is rotating at 7200 RPM and the mechanical power is 4 W, and the force on rotor is 4/2.377 or 0.0053 N. The torque on shaft is 0.0053 N·m at 2 A because of the assumed radius of the rotor (exactly 1 meter). Assuming a different radius would change the linear K_v but would not change the final torque result. To check the result, remember that power = torque·2π·angular speed/60.

So, a motor with 3600 K_v will generate 0.00265 N·m of torque per ampere of current, regardless of its size or other characteristics. This is exactly the value estimated by the K_T formula stated earlier.

References

↑ http://www.motioncomp.com/pdfs/Motor_Constant_Great_Equalizer.pdf
↑ http://learningrc.com/motor-kv/
1 2 3 "Mystery Motor Data Sheet" (PDF), hades.mech.northwest.edu
↑ "GENERAL MOTOR TERMINOLOGY" (PDF), www.smma.org
↑ "DC motor model with electrical and torque characteristics - Simulink", www.mathworks.co.uk
↑ "Technical Library > DC Motors Tutorials > Motor Calculations", www.micro-drives.com, archived from the original on 2012-04-04
↑ http://www.precisionmicrodrives.com/tech-blog/2014/02/02/reading-the-motor-constants-from-typical-performance-characteristics
↑ http://www.smma.org/pdf/SMMA_motor_glossary.pdf
↑ "DC motor starting and braking", iitd.vlab.co.in
↑ Understanding motor constants Kt and Kemf for comparing brushless DC motors

External links

"Development of Electromotive Force" (PDF), biosystems.okstate.edu, archived from the original (PDF) on 2010-06-04

This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.

[1] ttp://www.motioncomp.com/pdfs/Motor_Constant_Great_Equalizer.pdf

[2] ttp://learningrc.com/motor-kv/

[kk-3] 1 2 3 "Mystery Motor Data Sheet" (PDF), hades.mech.northwest.edu

[4] "GENERAL MOTOR TERMINOLOGY" (PDF), www.smma.org

[5] "DC motor model with electrical and torque characteristics - Simulink", www.mathworks.co.uk

[6] "Technical Library > DC Motors Tutorials > Motor Calculations", www.micro-drives.com, archived from the original on 2012-04-04

[7] ttp://www.precisionmicrodrives.com/tech-blog/2014/02/02/reading-the-motor-constants-from-typical-performance-characteristics

[8] ttp://www.smma.org/pdf/SMMA_motor_glossary.pdf

[9] "DC motor starting and braking", iitd.vlab.co.in

[10] Understanding motor constants Kt and Kemf for comparing brushless DC motors