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Vortex, manufacturer of the hugely popular Poker II 60% keyboard, has been teasing its next generation Poker on Facebook. Dubbed the POK3R, or Poker III, the new board is set to include several upgrades, and undoubtedly will sell for more than the Poker II’s ~$110 street price.
https://gamewap301.tumblr.com/post/663064105744220160/induction-motor-slot-pole-combinations. Optimal slot/pole and flux-barrier layer number combinations for synchronous reluctance machines Abstract: AC synchronous reluctance machine (SynRM) or permanent magnet assisted synchronous reluctance machine presently receives a great deal of interest, since there is less or even no rare earth permanent magnet in the rotor. I-B depicks a (3) phase (4) pole, (6) slot brushless motor with the coils wound around a single stator tooth the same as Figure I-A. Figure I-C is an (8) pole, (18) slot motor with (3) phases and a (2) slot coil winding pitch. Figure I-D is a common brushless configuration for (3) phase motors with (4) poles. The electromechanical characteristics of induction motors depend on the used stator and rotor slot combination. The correlation between the usage of different stator and rotor slot number combinations, magnetic flux density distributions, no-load iron losses and rated load winding over-temperatures for a specific induction motor is presented.
Here’s a quick rundown of the POK3R’s features–at least those we know so far, and how they stack up against the Poker II:
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Metal case: Unlike the Poker II, which ships with a plastic case, the POK3R will feature a low-profile cast aluminum case. This alone guarantees that the POK3R will retail for at least $150, and likely more. It appears to be the same aluminum case that Vortex has been selling separately for the last year or so.
Black or white: The POK3R will be available with black caps and a black case, or white caps and a white case, similar to the Poker II.
Full programmability with 3 layers: The Poker II has only two programmable layers with a fixed Pn key. Vortex says the Poker III will have three programmable layers with the Fn and Pn keys being programmable themselves–in other words, full programmability similar to keyboards with custom controllers.
Support for QWERTY, Dvorak, and Colemak: Vortex’s teaser photos suggest these layouts will be settable via DIP switches on the PCB, and DO show correct-profile Dvorak and Colemak keysets, but it’s unknown whether they will ship each layout as a separate SKU. When you start multiplying layout support with color, LED options, and so on… that makes a LOT of different SKUs, and retailers don’t like that–too difficult to stock everything. More on this below.
LED Backlighting with programmability: The Poker II comes in backlit and non-backlit varieties. The same will possibly be true of the POK3R, since some teaser shots show it with backlit-compatible keycaps and some show it with solid keycaps. However, all of the ‘naked’ Poker III shots so far have shown LEDs installed, so it might be a mandatory feature. Either way, we also know that on backlit models, you’ll also be able to program LEDs on a per-key basis if you only want certain keys illuminated. Note that it will NOT be an RGB board, although Vortex has commented that they’re interested in releasing RGB boards in the future when Corsair’s exclusivity contract ends.
Authentic Cherry MX switches: Unlike many of their competitors, Vortex won’t be switching to a lower-cost MX alternative switch like Kailh or Gateron.
Multiple types of keycaps, including PBT+POM doubleshots: In a Facebook comment, Vortex suggested that the Poker III will come with a choice of keycaps–including, at least, their recently released PBT keycaps with translucent doubleshot POM legends, dyesubbed PBT, lasered or printed PBT, and ABS (probably pad-printed).
Plate mounted: The POK3R will have a plate sandwiched between the PCB and switches for extra rigidity, just like the Poker 2. There was some previous speculation that it would be PCB-mounted (i.e., switches soldered directly to PCB with no plate in between) like the original Poker X, but this has since been proven false.
Revised function layer: On the Poker II’s function layer, the missing arrow keys were mapped to WASD. On the Poker III, they look to be mapped to IJKL instead, and many other functions have been relocated too. Of course, this is only the default configuration–with 3 programmable layers, you can arrange your function layer any way you want.
No “Enjoy Your Feeling” on the spacebar: Good, because no one enjoyed that on the Poker II.
Will be available in ISO: Good news for our European friends.
I think there are two main takeaways here.
First, the POK3R is going to be an expensive, high-end keyboard, with its aluminum case and vast new feature set. My guess is it’ll retail between $150 and $200, and probably closer to $200. If this happens, Vortex will continue to sell the Poker II as a “budget” option.
Second, Vortex is really pushing customizability, from color, to keycap material, to keycap layout, to backlighting. If you multiply together all the possibilities, you get dozens if not hundreds of combinations. There’s no way retailers will stock all these SKUs. It may mean that certain combinations are impossible to find at retail… or maybe Vortex is planning something special? Maybe they’re going to start selling made-to-order boards direct? That’ll be complicated since they’re based in Taiwan, but don’t rule it out completely–especially with the POK3R’s expected premium price.
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Finally, the latest word from Vortex is a February 2015 release date, though some people on the forums are saying March. Don’t hold your breath, though–Vortex is notorious for delays.
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I’ll close out here with a gallery of images Vortex has released so far. Enjoy, and let me know what your predictions are for the Poker III!
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https://gamewap301.tumblr.com/post/663064105744220160/induction-motor-slot-pole-combinations. The electromechanical characteristics of induction motors depend on the used stator and rotor slot combination. The correlation between the usage of different stator and rotor slot number combinations, magnetic flux density distributions, no-load iron losses and rated load winding over-temperatures for a specific induction motor is presented. I-B depicks a (3) phase (4) pole, (6) slot brushless motor with the coils wound around a single stator tooth the same as Figure I-A. Figure I-C is an (8) pole, (18) slot motor with (3) phases and a (2) slot coil winding pitch. Figure I-D is a common brushless configuration for (3) phase motors with (4) poles. An optimal stator and rotor pole numbers until 1. Feasible combinations for a three-phase FSPM machines with magnets are given in (1) 1. N s =6k 1,k 1 ∈ N∗ N r = N s ±k 2,k 2 ∈ N∗ (1) N s is the slot and magnet numbers, which must be even and N r is the rotor pole number. Thus, for a 12-slot machine, any rotor could potentially be. Optimal slot/pole and flux-barrier layer number combinations for synchronous reluctance machines Abstract: AC synchronous reluctance machine (SynRM) or permanent magnet assisted synchronous reluctance machine presently receives a great deal of interest, since there is less or even no rare earth permanent magnet in the rotor.
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Induction motor slot pole combinations list. The electromechanical characteristics of induction motors depend on the used stator and rotor slot combination. The correlation between the usage of different stator and rotor slot number combinations, magnetic flux density distributions, no-load iron losses and rated load winding over-temperatures for a specific induction motor is presented. I-B depicks a (3) phase (4) pole, (6) slot brushless motor with the coils wound around a single stator tooth the same as Figure I-A. Figure I-C is an (8) pole, (18) slot motor with (3) phases and a (2) slot coil winding pitch. Figure I-D is a common brushless configuration for (3) phase motors with (4) poles. Optimal slot/pole and flux-barrier layer number combinations for synchronous reluctance machines Abstract: AC synchronous reluctance machine (SynRM) or permanent magnet assisted synchronous reluctance machine presently receives a great deal of interest, since there is less or even no rare earth permanent magnet in the rotor. An optimal stator and rotor pole numbers until 1. Feasible combinations for a three-phase FSPM machines with magnets are given in (1) 1. N s =6k 1,k 1 ∈ N∗ N r = N s ±k 2,k 2 ∈ N∗ (1) N s is the slot and magnet numbers, which must be even and N r is the rotor pole number. Thus, for a 12-slot machine, any rotor could potentially be.
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Induction Motor Slot Pole Combinations
Induction Motor Slot Pole Combinations Diagram
Induction Motor Slot Pole Combinations List
Induction Motor Slot Pole Combinations Generator
Induction Motor Slot Pole Combinations Chart
The electromechanical characteristics of induction motors depend on the used stator and rotor slot combination. The correlation between the usage of different stator and rotor slot number combinations, magnetic flux density distributions, no-load iron losses and rated load winding over-temperatures for a specific induction motor is presented. Modulation motor is the world’s most innovative AC induction motor.Although it is basically a single-winding, two-speed squirrel cage motor, the PAM motor features one outstanding characteristic that makes it versatile in application and efficient in operation, especially where less than peak load operation is desired: the PAM motor does not. Hi There, I'm in the process of trying to design a 36 pole induction motor for one of our test beds in the factory. It'll be used to test a range of winches that we manufacture and by controlling this motor through a VSD we can perform certain tests without the primary gear box that gets fitted to the completed unit. Higher pole numbers. It is possible to find high winding factors by varying the slot pitch as studied in 2 or alternatively by finding a good combination between slot and pole numbers. This second approach is more challenging because of the high number of possible combinations when the pole number is high. It is investigated in this study.
There are many much more interesting questions related to the pole number of induction motors, e.g.: 1. Does the induction motor supplied by the main grid (say, 50 Hz) increases its torque capability in 'p' times with growing pole number 'p' since its speed decreases in 'p' time (like in a gearbox)? 2. Let's we have an induction motor with p=2 and feed it from 50 Hz grid. Then we re-connect the winding coils to arrange p=4 and feed if grow 100 Hz grid. Are performances of these two motors different or the same? Please note excluding frequency and inter-coil connections all remained the same. It depends on the required speed. n (rpm) = (60 x f) / N where:- f = frequency and N = number of pole pairs. The 60 is there to convert from revolutions per second to revolutions per minute as the frequency is in cycles per second. Pole pairs is there because that any pole must be constructed in a pairs top and bottom / left right, so with one cycle it will move half the distance. If you are using 50Hz and have a two pole motor 60 x 50 / 1 = 3000 rpm. The induction motor will run at a slight less speed due to 'slip' which is what gives the motor its torque. For example 5.5kW, 400v, 2 pole motor will run at approximately 2880 rpm. For a four pole machine, 60 x 50 / 2 = 1500 rpm so the same size motor at 5.5kW, 400v but 4 poles will have a nominal speed of 1500rpm but will run near 1455 rpm. When selecting a three phase motor, the number of poles is chosen to achieve the speed of rotation that you require. Here are two tables, one for a 50 Hz power supply and one for a 60 Hz power supply: The formula is n = 60 x f /p where n = synchronous speed; f = supply frequency & p = pairs of poles per phase. The actual running speed is the synchronous speed minus the slip speed. For a 50 Hz three phase supply:
2 poles or 1 pair of poles = 3,000 RPM (minus the slip speed = about 2,750 RPM or 6 -7% n) 4 poles or 2 pairs of poles = 1,500 RPM 6 poles or 3 pairs of poles = 1,000 RPM 8 poles or 4 pairs of poles = 750 RPM 10 poles or 5 pairs of poles = 600 RPM 12 poles or 6 pairs of poles = 500 RPM 16 poles or 8 pairs of poles = 375 RPM
For a 60 Hz three phase supply:
2 poles or 1 pair of poles = 3,600 RPM (minus the slip speed = about 2,750 RPM or 6 -7% n) 4 poles or 2 pairs of poles = 1,800 RPM 6 poles or 3 pairs of poles = 1,200 RPM 8 poles or 4 pairs of poles = 900 RPM 10 poles or 5 pairs of poles = 720 RPM 12 poles or 6 pairs of poles = 600 RPM 16 poles or 8 pairs of poles = 450 RPM
To determine the number of poles, you can read the data plate directly or calculate it from the RPM stated on the data plate or you can count the coils and divide by 3 (poles per phase) or by 6 (pairs of poles per phase). Where the power of the induction motor is constant, the torque increases at the rate that the speed decreases. With the advent of variable frequency drive (VFD), you can have any frequency / rated volts you desire. I often see name plates with things like 575VAC, 42.5 Hz etc. When these 'specials' are made I usually see 6 pole machines - but that may be just a manufacturer's preference.
Introduction
This article reviews the techniques to mitigate noise and vibrations due to magnetic forces in electrical machines (electromagnetically-excited noise and vibrations) based on EOMYS ENGINEERING consulting experience. The content of this article is taken from EOMYS technical trainings on electric motor NVH.
Noise and vibration control techniques of e-motors can be classified in three types:
reduction of the structural response independently of the electromagnetic excitations
reduction of the electromagnetic excitations independently of the structural response
reduction of the number of resonances occuring between electromagnetic excitations and structural modes
The most efficient acoustic noise mitigation techniques are based on the cancellation of the harmonic electromagnetic excitations responsible for vibration and noise.
All these noise control techniques can be applied at early electromagnetic design stage using MANATEE software for the fast calculation of noise and vibrations in electric motors.
Choice of the topology
There is no unique choice for a low noise & vibration machine, but some topologies are more challenging in terms of NVH. This also depends on the application constraints (e.g. power density, fixed speed or variable speed application).
Outer rotor topologies (also called outrunner motor if it is a brushless DC motor) can lead to higher noise & vibration due to rotor yoke lower stiffness compared to an outer stator topology. Fractional-slot winding or more particularly concentrated or tooth winding might lead to higher acoustic noise & vibrations compared to integral distributed winding due a higher number of wavenumbers in the armature field and the possible presence of subharmonics.
The best armature winding is the one creating the most sinusoidal mmf, so the double-layer, shorted-pitch, distributed integral winding. For permament magnet rotors, the best magnet architecture is also the one creating the most sinusoidal rotor mmf, so either Hallbach configuration for surface magnets, or multi-barriers V-shape interior magnets with bread-loaf pole shapes (also called sinusoidal field poles).
MANATEE software can be used to calculate the NVH behaviour of all types of radial flux electric machines, including interior (buried), inset and surface permanent magnet synchronous machines, squirrel cage induction machines, outer rotor and inner rotor electrical machines.New topologies can be easily implemented upon request.
Machine SPMSM_015 Topology
Asymmetries
An electric machine designed to have low harmonic distortion rate magnetomotive forces (e.g. an IPMSM with double-layer shorted-pitch distributed-winding, and V-shaped magnets) can reveal noisy due to manufacturing & assembly tolerances which introduce asymmetries.
Static and dynamic eccentricities increase the spectral density (wavenumbers & frequencies) of harmonic magnetic forces.
Mass & stiffness asymetries (and low number of teeth, introducing discrete distribution of stiffness along yoke) increase the modal density and number of resonances at variable speed.
Uneven airgap modulates magnetic forces and increases the number of different force wavenumbers, increasing the number of structural resonances.
Effect of asymmetries on electromagnetically-excited noise using MANATEE software (left: no asymmetry, right: with asymmetries)
To lower noise and vibrations the machine should be magnetically and geometrically symmetrical:
low tolerance on eccentricities and misalignments
low tolerance on lamination roundness
low tolerance on magnet magnetization dispersion
low tolerance on magnet position in slots
MANATEE software can consider the NVH effect of radial and conical eccentricities, as well as uneven airgap, demagnetization, and pole displacement.
Choice of the pole / slot / phase numbers
Generalities
Increasing the number of slot per pole per phase reduces the harmonic density of airgap flux and resulting magnetic forces.
Increasing the number of pole pairs gives a lower electromagnetic yoke height, thus higher vibration & noise. However, the lowest force wavenumber is also given by the Greatest Common Divider between stator slot and pole numbers in Permanent Magnet Synchronous Machines: increasing p also potentially increases GCD(Zs,2p), resulting in lower electromagnetic vibrations.
These examples show that changing the slot/pole/phase combination involves different electromagnetic and vibro-acoustic opposite effects, so numerical simulation with MANATEE software is advised.
Induction Motor Slot Pole Combinations Diagram
Case of induction machines
The number of rotor slots Zr is a key design parameter as it influences both wavenumbers and frequencies of Maxwell harmonic forces. Pole/slot interactions in induction machines create exciting forces at multiples of the rotor slot passing frequency.
Some empirical rules to choose the slot / pole combination are given in many electrical engineering books such as (1-5). However these rules are continuous, they do not reflect correctly the discrete nature of harmonic force wave and do not account for the stator natural frequencies nor the speed range of the machine. The use of such empirical rules should be avoided and numerical simulation is advised for instance with MANATEE software. An example of the discrete evolution of electromagnetically-excited noise with rotor slot number is given in this tutorial.
Effect of the rotor bar number on the maximum sound level emitted by a variable-speed induction motor (MANATEE software output)
When both stator slot and rotor slot numbers Zs & Zr are even integers, Maxwell force harmonics only contain even force wavenumbers for integral windings, thus avoiding Unbalance Magnetic Pull.
The number of rotor and stator slots should never be equal, otherwise strong pulsating radial and tangential force waves appear in the machine, creating high air-borne noise the stator breathing mode and potentially high structure-borne noise due to torque ripple.
Contrary to Permanent Magnet Synchronous Machines where some global rules on slot / pole combination can be relevant, the case of induction machines is more complex. Ideally one should avoid the presence of high magnitude (due to first rank of permeance), 'low' wavenumber so in particular one should avoid
(Zr-Zs|=0, 2 or 4
|Zr-Zs-2p|=0, 2 or 4
|Zr-Zs+2p|=0, 2 or 4
Relying only these rules of thumbs for the design of an electric machine is suboptimal and risky. Again variable speed calculation of electromagnetically-excited noise is advised using MANATEE software.
Case of synchronous machines
When stator slot is an even integers, Maxwell force harmonics only contain even force wavenumbers for integral windings, thus avoiding Unbalance Magnetic Pull. More precisely UMP only exists if |Zs-2p|=1.
Maximization of LCM(Zs,2p) increases the frequency of open-circuit pulsating (wavenumber r=0) radial and tangential force harmonics (in particular cogging torque and average radial force).
Minimization of GCD(Zs,2p) reduces the magnitude of open-circuit pulsating (wavenumber r=0) radial and tangential force harmonics (in particular cogging torque and average radial force).
Maximization of GCD(Zs,2p) increases the non-zero wavenumbers of open-circuit (and probably also partial load) magnetic forces, thus potentially reducing noise and vibration levels.
Simiarly to induction machines, one should avoid the presence of high magnitude (due to first rank of permeance), 'low' wavenumber so in particular one should avoid
(2p-Zs|=0, 2
The 12s10p PMSM machine is known to be prone to high vibration and noise because |2p-Zs|=2: in open-circuit and under commutation, many force harmonics have a wavenumber 2 and can resonate with the stator elliptical mode.
As you can see some of these rules of thumb are contradictory and changing the slot number also changes the magnitude of permeance harmonics, so full NVH variable speed simulation is recommended with MANATEE software.
Choice of the winding
The ideal winding gives a sinusoidal mmf, it has an infinite number of phases ( no « belt harmonics »), an infinite number of slots (no « slot harmonics » or preferably no « step harmonics ») or no slot at all ('airgap winding').
To avoid Unbalanced Magnetic Pull the winding-induced mmf should never have two harmonics separated of 1.
Concentrated winding / tooth-winding / fractional winding have the largest mmf distortion factor, however if properly designed they do not generate noise & vibrations.
Shorted-pitch distributed windings gives the smoothest magnetomotive force.Short-pitching or chording technique consists in having several winding layers and shifting the winding pattern in each layer. The chording cannot reduce the largest mmf step harmonics at Zs-p and Zs+p space harmonics.The coil pitch Y (in slots, between 0 and Zs/(2p)-1) can be chosen as (5/6) Zs/(2p) to reduce the stator mmf space harmonics 5p and 7p.
This MANATEE software tutorial explores the effect of short pitch on magnetic noise of an induction motor.
Example of an AC winding distribution (MANATEE output)
All winding types can be modelled in MANATEE software, using automated winding algorithms, winding connection matrix or Koil winding freeware. Dedicated post-processing allow to analyze the armature field harmonic content are available (see for instance plot_smmf_space).
Skewing
Skewing consists in rotating a 2D slice of the electrical machine along its rotation axis in order to smoothen the average field and cancel out some specific harmonics. Skewing can be applied to stator, rotor or both.
Stator skew is generally linear, and rotor skew depends on machine topology (linear for squirrel cages, stepped-skew or linear for permanent magnets).
Skewing can cancel a given force harmonics when considering its average longitudinal value (DC component). However, it also introduces an axial magnetic force variation and can therefore excite longitudinal structural modes of the stator and rotor structures. It can also create an additional axial thrust.
The skewing angle and the part to be skewed (rotor or stator) depends on the magnetic force harmonic to be cancelled.
The best skewing angle might be different when trying to minimize torque harmonics or radial force harmonics, and the best skewing angle might depend on the load condition.
This task can be carried using MANATEE simulation environment where all types of skew shape can be modelled. This tutorial of MANATEE shows how to calculate the effect of rotor skew on torque ripple and acoustic noise.
Effect of the rotor skew rate on the maximum sound power level radiated by a variable-speed PMSM (MANATEE software output)
Pole magnetization
Playing on the magnetization pattern allows to tune the rotor mmf harmonic content and thereof influence the vibroacoustic behaviour of the electric motor.Hallbach pattern lowers the spatial harmonic content of mmf but is expensive to manufacture.Shaping the magnetization pattern and optimizing the pole dimensions to minimize some specifics harmonics involved in noise generation is not sufficient to obtain a low vibration and noise design, as some other harmonics may increase during this process, creating new resonances.
A full electromagnetic and NVH simulation is recommended with MANATEE software. MANATEE software includes radial, parallel and Hallbach magnetization patterns in both subdomain magnetic models and finite element models.
Pole shaping
Magnet / pole shoe shaping allows to « tune » the rotor mmf harmonic content and thereof the vibroacoustic behaviour of the electric machine.
As both constructive and destructive interference occurs, cancelling a given magnet mmf space harmonic responsible for acoustic noise does not necessarily reduce noise as it can increase other force harmonics.For wound rotor synchronous machines the pole arc curvature has large influence on noise.Due to the combined effect of radial and tangential forces on radial vibrations and noise, simulation with MANATEE software is recommended.MANATEE sensitivity tools and optimization tools can be used for instance to find the best magnet pole arc to pole pitch ratio minimizing both torque ripple and acoustic noise.
Pole width and position
The pole widths or pole positions (pole shifting technique) of a synchronous machine can also be modulated to tune the rotor magnetimotive force spectrum content. Other pole displacement techniques to reduce cogging torque and zero-th average radial force include axial and radial pole-pairing technique (association of two different pole shapes to cancel a given harmonic).
Pole displacement techniques should be applied very carefully and should not focus only on the minimization of torque ripple / cogging torque, as noise and vibrations are also produced by higher wavenumber tangential and radial force harmonics. Simulation with MANATEE software is recommended.
Slot and tooth shape / position
Stator slot shapes or positions can be modulated to spread the permeance spatial spectrum or reduce / cancel a specific harmonic involved in noise and vibration generation.Slot-pairing (teeth pairing) techniques can reduce cogging and average radial forces by cancelling the first component only at LCM(Zs,2p)fR.
Notches
Notches (sometimes called circumferential slits, auxiliary slots, dummy slots, or grooves) consists in removing some part of the magnetic sheet material to modulate the airgap reluctance.If properly sized, notching can artificially increase the permeance wavenumber, as if the slot number was increased.The average airgap is increased due to notches (increase of Carter coefficient) so it may slightly reduce the electromagnetic performances.The introduction of notches can also increase the local saturation level.Similarly to skewing, the effect of notches can strongly depend on the operating point.
Simulation with MANATEE software is recommended. This MANATEE tutorial demonstrates how to use rotor notches to reduce the acoustic noise of an induction machine.
FEMM submodel to calculate a rotor notch effect
Stator slot opening optimization
The permeance harmonics are due to reluctance variation along the airgap, and slotting effects are a source of permeance harmonics at multiples of slot number. Slot to tooth opening ratio can reduce some of the permeance harmonics (similarly to pole pitch to pole arc ratio for the rotor mmf), but it is influenced by saturation and sometimes several slotting harmonics are involved in noise generationIf the first stator slot harmonic (ks=1) is responsible for a force wave in a machine - ex: PMSM with Zs=12 and p=5, a harmonic force exists with r=(1*Zs-1*p)-(0+1*p)=2 - closing the slot will cancel the permeance harmonic.
In practice slots cannot be geometrically closed due to winding process (a minimum slot opening is often required to pass needle and strand, or to use tooth tip as a support for winding) and magnetically closed due to saturation.
Optimal slot design can be carried using MANATEE software for the prediction of electromagnetic noise and vibraitons.
Magnetic wedges
Magnetic wedges allow to reduce the magnetic reluctance change in the slot opening, reducing flux density slotting harmonics and therefore cogging torque and all magnetic force harmonics related to permeance harmonics.Due to low relative permeability of commercial wedges (max 10) the effect on noise is limited (max 3 dB).The impact of magnetic wedges on e-motor vibroacoustics can be studied within MANATEE e-NVH software.
Airgap increase
Electromagnetic performances (e.g. efficiency) is directly affected by airgap width so one must check that the impact on performance and control does not worsen the noise (e.g. due to higher current).Airgap increase can affect differently magnetic force harmonics, and the effect on magnetic noise is quite limited.The effect of airgap width can be easily studied using MANATEE software parameter sweep environment.
Flux barriers
Flux barriers or pockets in stator yoke and teeth, or rotor yoke and teeth can modify the airgap flux harmonic content and magnetic force magnitude due to local saturation effects.It generally significantly affects the machine performances (increase of leakage inductance, reduction of torque) so it must be used carefully.
Effects of flux barrier dimensions on the harmonic content of airgap flux obtained with MANATEE software
MANATEE software can be used to size the flux barriers as shown in this validation article.
Control
Case of induction machines
Magnetic noise is linked to magnetizing flux and not to torque, it is possible to increase torque with constant flux and noise.MANATEE software simulation allows to find the trade-offs between vibroacoustic and electrical performances.
Case of synchronous machines
Current angle or load angle has a strong influence on average magnetic force magnitude.The load angle can influence the magnitude of higher time harmonics of wavenumber r=0 tangential & radial forces. The load angle evolution of force harmonics depends on their frequency and spatial order. Iq changes both pulsating radial and tangential force harmonics (torque), while Id mainly changes pulsating radial force harmonics. NField weakening (negative Id ) may reduce pulsating radial force ripple while increasing tangential force ripple.
A detailed sensitivity analysis including structure-borne and air-borne noise under MANATEE software is advised to study the tradeoffs between optimal control for efficiency and optimal control for noise reduction.
Harmonic current injection
Generalities
A given vibration harmonic can be compensated by injecting additional harmonic currents, depending on the magnetic force wavenumber to be cancelled.As the current modulates the spatial harmonics of mmf winding functions, the current injection cannot create new wavenumbers than those already present in the magnetic forces. Current injection introduces new time harmonics and therefore new force harmonics (cf PWM lines), one must check that this does not worsen the vibration or noise level nor torque ripple.
High frequency noise is more difficult to damp with current injection (requires higher controller bandwith & higher reactance can induce higher DC bus voltage)Harmonic injection at 6f in DQH frame can damp r=0 pulsating harmonic force at 6f.
Synchronous machines
For synchronous machines, pulsating radial / tangential force waves magnitude at frequencies proportional to LCM(Zs,2p)fs/p can be damped using current injection. For radial force damping either Id or Iq harmonic injection theoretically works.
Induction machines
Radial force harmonics of wavenumbers 0 and 2p can be damped using current injection. For other wavenumbers, a detailed study must be carried.MANATEE software includes a special e-NVH mitigation environment to optimize harmonic current injection with respect to acoustic noise and torque ripple.
Switching strategies
Induction Motor Slot Pole Combinations List
Generalities
Induction Motor Slot Pole Combinations Generator
Voltage inverter switching strategies determine phase voltage harmonic content and resulting phase current spectrum. Supply voltage harmonics contain harmonics linked to the inverter Pulse Width Modulation (PWM) switching frequency (ex: fswi, 2fswi) and harmonics linked to fundamental (ex: 5f, 7f). The largest voltage, current, forces, vibration and noise harmonics can occur around once or twice the switching frequency depending on the PWM strategy and torque/speed operating point of the machine.
A voltage harmonic f creates a harmonic current f which in turn generates magnetic forces and vibration waves f+fs, 2p and f-fs, 0 where fs is the fundamental electrical frequency.
Increasing the switching frequency generally reduces the acoustic noise (dBA reduction above 2.5 kHz), in some cases it can be chosen out from human’s ear sensitivity. However, it significantly increases inverter losses so again tradeoffs between efficiency and NVH must be analyzed, which can be carried under MANATEE software.
Spread spectrum strategies
Spread spectrum principle is already used in aerodynamic noise (uneven blade spacing of fans). The same principle is used in randomized switching strategies.Such strategies may lower the maximum dBA level, but they result in a wider excitation spectrum which can lead to new resonances depending on damping and natural frequency position with respect to exciting forces. Finally, random strategies can significantly affect sound perception and a detailed sound quality study is advised.MANATEE software includes some sound quality metrics to study this effect.
PWM strategies
There exist a number of PWM strategies such as SPWM, SVPWM, DPWM0, DPWM1, DPWM2, DWPM3, DPWMmin, DPWMmax, GDPWM.These commutations strategies have been developed to maximize converter output and efficiency, and they change the excitation voltage spectra and resulting sound power level as well as sound quality metrics.All these PWM strategies are already implemented in MANATEE e-NVH software, which also includes sound quality metrics to optimize power electronics switching strategy.
Structural response
Lower noise & vibration can be achieved by putting natural frequencies further away from magnetic excitations.Stator yoke can be stiffened to reduce vibration and noise levels ; in this case one must check that the natural frequency change due to the yoke geometry change does not compensate noise and vibration reduction due to yoke stiffening.
Induction Motor Slot Pole Combinations Chart
MANATEE software can be used to automatically study the effect of lamination shape on acoustic noise.
Other techniques to play on both air-borne and structure-borne noise include
optimize yoke geometry
optimize coupling between lamination and housing
optimize slot stiffness (winding material, spacers)
optimize stator fixation method in casing
MANATEE software coupled to FEA can be used to optimize these couplings and find a way to reduce the overall noise levels considering all transfer paths.
Damping
Increasing damping is one of the most efficient techniques to reduce noise and vibration of electric machines. It includes:
optimization of impregnation process (VPI, potting, dipping): materials, curing process, operating temperature
use of higher damping magnetic sheets
use of interlamination damping
use of viscoelastic materials
References
(1) J.F. Gieras, C. Wang and J.C. Lai, Noise of polyphase electric motors, CRC Press, 2005.
(2) P.L. Timar, Noise and vibration of electrical machines, Elsevier, 1989.
(3) S.J. Yang, Low noise electrical motors, Clarendon Press, Oxford, 1981.
(4) PYRHONEN Juha, Tapani Jokinen, Valéria Hrabovcova, Design of Rotating Electrical Machines (2nd Ed.), Wiley, 2013
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Piaggio Vehicles Pvt Ltd (PVPL) has announced the launch of its 6 feet deck length diesel cargo named Ape Xtra LDX +. The vehicle comes with a 599 cc diesel engine with a 5+1 gearbox and the. Piaggio Ape Auto DXL three wheeler for commercial purpose and I easily ride 3 passenger at once, its available in Diesel.
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Wikipedia: http://en.wikipedia.org/wiki/Piaggio_Ape
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Anglicky (český popis chybí)
The Piaggio Ape ((ˈpjaddʒo ˈaːpe); ah-pay;(not in citation given)Italian for bee), sometimes referred to as Ape Piaggio, Apecar, Ape Car or just Ape, is a three-wheeled light commercial vehicle produced since 1948 by Piaggio.
The vehicles come in various configurations such as vans and pickups for load carrying (popular with postal administration in some countries) and an autorickshaw for human transportation (Tukxi). More recently Piaggio have made lifestyle models such as the Ape Cross Country and the Ape Web aimed at the young. The Ape is also commonly used as a promotion tool. Advertising hoardings are mounted in the load bay. The Ape's unusual looks can help draw attention to a brand or business.
The Ape is still not an uncommon sight in Italy where its compact size allows it to negotiate narrow city streets and park virtually anywhere. In small southern villages, it is also often seen at the roadside where the load area is used as an impromptu market stall by farmers.
Most Apes are produced in India by Piaggio India, and a similar vehicle is manufactured by Bajaj Auto. In India the Ape is most commonly found in the form of an autorickshaw. A relatively small number of Apes is still made in Italy. On October 16, 2013, Piaggio announced that the production of Ape would be completely shut down in Italy and entirely moved to India.
Nowadays two model ranges are offered: the 'Ape 50' with a 49.8 cc petrol engine and the larger 'Ape TM' which comes available with a 218 cc petrol engine or a 422 cc diesel engine. The 'Ape 50' can carry 175 to 205 kg (386 to 452 lb) while the 'TM' and 'Classic' can carry 700 to 805 kg (1,543 to 1,775 lb) (depending on version and engine). Fuel consumption for the current Ape 50 model is about 30 km/l (85 mpg-imp; 71 mpg-US) A limited edition named the Calessino was made available: this had retro styling and came in an autorickshaw body. The bodywork was close to the Ape of the 1950s and 1960s and was designed to evoke memories of the era of dramatic economic growth in Italy known as Miracolo Economico.
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Výkon motoru 1.1 kW (1 PS) . Maximální rychlost 50 km/h. Hmotnost 270 kg. Palivo benzín. 4-rychlostní Manuální převodovka. Motor 498 ccm (30 cui), TL4T.
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Ape 50 TM valník o obsahu 50 ccm z roku 1985 né zrovna krasavec ale právě renovuji do původního stavu.
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Ape Piaggio Poker Diesel Parts
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