Mechanics of planar particle motion: Difference between revisions

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{{Modulation techniques}}
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'''Space vector modulation''' ('''SVM''') is an algorithm for the control of [[pulse width modulation]] (PWM).<ref name=control>
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{{cite book
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| author = M.P. Kazmierkowski, R. Krishnan, and F. Blaabjerg
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| title = Control in Power Electronics: Selected Problems
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| url = http://books.google.com/books?id=6_dmMHEyvrkC&pg=PA373&dq=%22space+vector+modulation%22+intitle:%22Control+in+Power+Electronics%22&lr=&as_brr=0&as_pt=ALLTYPES&ei=CBWOSdCVDJO2ygTvxuiXBg
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}}</ref> It is used for the creation of [[alternating current]] (AC) [[waveform]]s; most commonly to drive [[3 phase]] AC powered motors at varying speeds from DC using multiple [[Switching amplifier|class-D amplifiers]]. There are various variations of SVM that result in different quality and computational requirements. One active area of development is in the reduction of [[total harmonic distortion]] (THD) created by the rapid switching inherent to these algorithms.


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==Principle==
 
[[File:Three leg inverter.gif|240px|thumb|right|Topology of a basic three phase inverter.]]
 
A three phase inverter as shown to the right converts a DC supply, via a series of switches, to three output legs which could be connected to a three-phase motor.
 
The switches must be controlled so that at no time are both switches in the same leg turned on or else the DC supply would be shorted. This requirement may be met by the complementary operation of the switches within a leg. i.e. if A<sup>+</sup> is on then A<sup>−</sup> is off and vice versa. This leads to eight possible switching vectors for the inverter, V<sub>0</sub> through V<sub>7</sub> with six active switching vectors and two zero vectors.
 
<center>
{| class="wikitable" border="1"
|-
! Vector
! A<sup>+</sup>
! B<sup>+</sup>
! C<sup>+</sup>
! A<sup>−</sup>
! B<sup>−</sup>
! C<sup>−</sup>
! V<sub>AB</sub>
! V<sub>BC</sub>
! V<sub>CA</sub>
!
|-
| V<sub>0</sub> = {000}
| align="center"| OFF
| align="center"| OFF
| align="center"| OFF
| align="center"| ON
| align="center"| ON
| align="center"| ON
| align="center"| 0
| align="center"| 0
| align="center"| 0
| zero vector
|-
| V<sub>1</sub> = {100}
| align="center"| ON
| align="center"| OFF
| align="center"| OFF
| align="center"| OFF
| align="center"| ON
| align="center"| ON
| align="center"| +V<sub>dc</sub>
| align="center"| 0
| align="center"| −V<sub>dc</sub>
| active vector
|-
| V<sub>2</sub> = {110}
| align="center"| ON
| align="center"| ON
| align="center"| OFF
| align="center"| OFF
| align="center"| OFF
| align="center"| ON
| align="center"| 0
| align="center"| +V<sub>dc</sub>
| align="center"| −V<sub>dc</sub>
| active vector
|-
| V<sub>3</sub> = {010}
| align="center"| OFF
| align="center"| ON
| align="center"| OFF
| align="center"| ON
| align="center"| OFF
| align="center"| ON
| align="center"| −V<sub>dc</sub>
| align="center"| +V<sub>dc</sub>
| align="center"| 0
| active vector
|-
| V<sub>4</sub> = {011}
| align="center"| OFF
| align="center"| ON
| align="center"| ON
| align="center"| ON
| align="center"| OFF
| align="center"| OFF
| align="center"| −V<sub>dc</sub>
| align="center"| 0
| align="center"| +V<sub>dc</sub>
| active vector
|-
| V<sub>5</sub> = {001}
| align="center"| OFF
| align="center"| OFF
| align="center"| ON
| align="center"| ON
| align="center"| ON
| align="center"| OFF
| align="center"| 0
| align="center"| −V<sub>dc</sub>
| align="center"| +V<sub>dc</sub>
| active vector
|-
| V<sub>6</sub> = {101}
| align="center"| ON
| align="center"| OFF
| align="center"| ON
| align="center"| OFF
| align="center"| ON
| align="center"| OFF
| align="center"| +V<sub>dc</sub>
| align="center"| −V<sub>dc</sub>
| align="center"| 0
| active vector
|-
| V<sub>7</sub> = {111}
| align="center"| ON
| align="center"| ON
| align="center"| ON
| align="center"| OFF
| align="center"| OFF
| align="center"| OFF
| align="center"| 0
| align="center"| 0
| align="center"| 0
| zero vector
|}
</center>
Note that looking down the columns for the active switching vectors V<sub>1-6</sub>, the output voltages vary as a pulsed sinusoid, with each leg offset by 120 degrees of [[Phasor_(electronics)|phase angle]].
 
To implement space vector modulation a reference signal V<sub>ref</sub> is sampled with a frequency f<sub>s</sub> (T<sub>s</sub> = 1/f<sub>s</sub>). The reference signal may be generated from three separate phase references using the [[Alpha beta gamma transform|<math>\alpha\beta\gamma</math> transform]]. The reference vector is then synthesized using a combination of the two adjacent active switching vectors and one or both of the zero vectors. Various strategies of selecting the order of the vectors and which zero vector(s) to use exist. Strategy selection will affect the harmonic content and the switching losses.
 
[[File:Space Vector Modulation.gif|center|thumb|400px|All eight possible switching vectors for a three-leg inverter using space vector modulation. An example V<sub>ref</sub> is shown in the first sector. V<sub>ref_MAX</sub> is the maximum amplitude of V<sub>ref</sub> before non-linear overmodulation is reached.]]
 
More complicated SVM strategies for the unbalanced operation of four-leg three-phase inverters do exist. In these strategies the switching vectors define a 3D shape (a hexagonal [[Prism (geometry)|prism]] in <math>\alpha\beta\gamma</math> coordinates<ref>R. Zhang, V. Himamshu Prasad, D. Boroyevich and F.C. Lee, "Three-Dimensional Space Vector Modulation for Four-Leg Voltage-Source Converters," IEEE Power Electronics Letters, vol. 17, no. 3, May 2002</ref> or a [[dodecahedron]] in abc Three-Dimensional Space Vector Modulation in abc coordinates<ref>M.A. Perales, M.M. Prats, R.Portillo, J.L. Mora, J.I. León, and L.G. Franquelo, "Three-Dimensional Space Vector Modulation in abc Coordinates for Four-Leg Voltage Source Converters," IEEE Power Electronics Letters, vol. 1, no. 4, December 2003</ref>) rather than a 2D [[hexagon]].
 
==See also==
 
* [[Alpha beta gamma transform|<math>\alpha\beta\gamma</math> transform]]
* [[Inverter (electrical)]]
* [[pulse width modulation]]
 
==References==
 
{{reflist}}
 
==External links==
*[http://www.vissim.com/solutions/field_oriented_motor_control.html Model based control of PMSM motor with space vector modulation] Description and working [[VisSim]] source code diagram.
 
{{DEFAULTSORT:Space Vector Modulation}}
[[Category:Electrical engineering]]
[[Category:Electronics]]

Revision as of 18:11, 17 January 2014

Template:Modulation techniques Space vector modulation (SVM) is an algorithm for the control of pulse width modulation (PWM).[1] It is used for the creation of alternating current (AC) waveforms; most commonly to drive 3 phase AC powered motors at varying speeds from DC using multiple class-D amplifiers. There are various variations of SVM that result in different quality and computational requirements. One active area of development is in the reduction of total harmonic distortion (THD) created by the rapid switching inherent to these algorithms.

Principle

Topology of a basic three phase inverter.

A three phase inverter as shown to the right converts a DC supply, via a series of switches, to three output legs which could be connected to a three-phase motor.

The switches must be controlled so that at no time are both switches in the same leg turned on or else the DC supply would be shorted. This requirement may be met by the complementary operation of the switches within a leg. i.e. if A+ is on then A is off and vice versa. This leads to eight possible switching vectors for the inverter, V0 through V7 with six active switching vectors and two zero vectors.

Vector A+ B+ C+ A B C VAB VBC VCA
V0 = {000} OFF OFF OFF ON ON ON 0 0 0 zero vector
V1 = {100} ON OFF OFF OFF ON ON +Vdc 0 −Vdc active vector
V2 = {110} ON ON OFF OFF OFF ON 0 +Vdc −Vdc active vector
V3 = {010} OFF ON OFF ON OFF ON −Vdc +Vdc 0 active vector
V4 = {011} OFF ON ON ON OFF OFF −Vdc 0 +Vdc active vector
V5 = {001} OFF OFF ON ON ON OFF 0 −Vdc +Vdc active vector
V6 = {101} ON OFF ON OFF ON OFF +Vdc −Vdc 0 active vector
V7 = {111} ON ON ON OFF OFF OFF 0 0 0 zero vector

Note that looking down the columns for the active switching vectors V1-6, the output voltages vary as a pulsed sinusoid, with each leg offset by 120 degrees of phase angle.

To implement space vector modulation a reference signal Vref is sampled with a frequency fs (Ts = 1/fs). The reference signal may be generated from three separate phase references using the transform. The reference vector is then synthesized using a combination of the two adjacent active switching vectors and one or both of the zero vectors. Various strategies of selecting the order of the vectors and which zero vector(s) to use exist. Strategy selection will affect the harmonic content and the switching losses.

All eight possible switching vectors for a three-leg inverter using space vector modulation. An example Vref is shown in the first sector. Vref_MAX is the maximum amplitude of Vref before non-linear overmodulation is reached.

More complicated SVM strategies for the unbalanced operation of four-leg three-phase inverters do exist. In these strategies the switching vectors define a 3D shape (a hexagonal prism in coordinates[2] or a dodecahedron in abc Three-Dimensional Space Vector Modulation in abc coordinates[3]) rather than a 2D hexagon.

See also

References

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  2. R. Zhang, V. Himamshu Prasad, D. Boroyevich and F.C. Lee, "Three-Dimensional Space Vector Modulation for Four-Leg Voltage-Source Converters," IEEE Power Electronics Letters, vol. 17, no. 3, May 2002
  3. M.A. Perales, M.M. Prats, R.Portillo, J.L. Mora, J.I. León, and L.G. Franquelo, "Three-Dimensional Space Vector Modulation in abc Coordinates for Four-Leg Voltage Source Converters," IEEE Power Electronics Letters, vol. 1, no. 4, December 2003