class: center, middle # EE-568 Selected Topics in Electrical Machines ## Ozan Keysan [keysan.me](http://keysan.me) Office: C-113
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Tel: 210 7586 --- # Permanent Magnets Machines
### Becoming more and more popular with high efficiency and high torque density --- #Applications
--- # History
--- # Neodymium Magnets (NdFeB) ### Strongest and most common (60% market share) ### Neodmymium is mostly exported by China ### Expensive (600 TL/kg, $85/kg) (2020)
--- # Magnetization Directions
--- #B-H Curve of a Magnet -- ### Desired Properties: -- ### Large Remanence flux density (retentivity, point that crosses B axis) -- ### Large [coercivity](http://hyperphysics.phy-astr.gsu.edu/hbase/solids/imgsol/coercivity.gif) (point that crosses H axis) -- ![](https://www.electronics-tutorials.ws/wp-content/uploads/2013/08/mag20.gif) --- # Magnet Strength Comparison
--- ## Intrinsic vs Normal B-H Charateristics
### We can only measure normal curve [More info about magnets](http://what-when-how.com/electric-motors/hard-magnetic-materials-permanent-magnets-electric-motors/), [Magnet Guide](http://www.allianceorg.com/pdfs/Magnet_Tutorial_v85_1.pdf), [Demagnetization](http://www.shinetsu-rare-earth-magnet.jp/e/design/) --- # Demagnetization of PMs
### If external magnetic fields get below the knee point, PM will lose strength --- # Demagnetization of PMs ## Recoil Line ### Magnets will loose strength if the reverse magnetic field goes beyond the knee point.
--- # Magnets with Temperature ### Real Datasheet of Sm-Co (Samarium-Cobalt Magnet)
### Magnets become less stable with increasing temperature. --- # What is Magnetic Force? ### [Why magnets attract each other?](http://www.youtube.com/watch?v=uTcuDprmues) by Richard Feynman -- ### [Magnets and Special Relativity](https://www.youtube.com/watch?v=1TKSfAkWWN0) Reading Suggestion: [Eminim Şaka Yapıyorsunuz Bay Feynman](http://www.idefix.com/Kitap/Eminim-Saka-Yapiyorsunuz-Bay-Feynman-Merakli-Bir-Sahsiyetin-Maceralari/Richard-P-Feynman/Bilim/Populer-Bilim/urunno=0000000427673)
--- # Magnetic Circuits with Magnets, Load Line
[More info on load lines](https://ocw.mit.edu/courses/electrical-engineering-and-computer-science/6-061-introduction-to-electric-power-systems-spring-2011/readings/MIT6_061S11_ch11.pdf), --- # Magnetic Circuits with Magnets, Load Line ## Be aware of the temperature variation
# The magnet can lose some of its strength --- # Magnet Grades ## A definition for its strength (i.e. max. stored energy)
--- # Magnet Grades
--- # Magnet Grades ## Last letter defines the working temperature - ## No Letter: < 80 C -- - ## M: Medium, <100 C -- - ## H: High, <120 C -- - ## SH: Super High, <150 C --- # Magnet Coatings ### Beware NdFeB magnets are prone to corrosion and need to be coated --
--- # Modelling of Magnets ## Operation range of a magnet
--- # Modelling of Magnets ## Equivalent Circuit (Flux Source)
--- # Modelling of Magnets ## Thevenin Equivalent Circuit (MMF Source)
--- # Modelling of Magnets ## If the magnet is operating in linear region ### \\(B_m = B_r + \mu_R \mu_0 H_m \\) ### \\(H_m\\) is negative (third quadrant in BH graph) -- ### \\(\Phi = B_m A_m \\) -- \\(\ = B_r A_m + \mu_R \mu_0 A_m H_m \\) -- ### \\(\Phi = B_m A_m \\) -- \\(\ = \Phi_r + \dfrac{F_m}{R_m} \\) --- # Modelling of Magnets ### \\(\Phi = \Phi_r + \dfrac{F_m}{R_m} \\) -- ### A constant flux source with a reluctance in parallel (i.e Norton circuit) ### \\(R_m = \dfrac{l_m}{ \mu_0 \mu_r A_m} \\) ### \\(P_m = \dfrac{1}{R_m} \\): Permeance --- ## Thevenin Equivalent Circuit (MMF Source)
### Magnet can be considered as a coil (MMF source) with: ### \\(NI =\\) -- \\(\Phi_r R_m =\\) -- \\(B_r A_m \dfrac{l_m}{\mu_o \mu_r A_m} \\) -- \\(= \dfrac{B_r l_m}{\mu_o \mu_r} \\) --- # Group Exercise-#1 --
### Calculate the airgap flux density for: --- # Group Exercise- #2 --
### Draw the magnetic equivalent circuit (ignore leakage) --- # Group Exercise- #2 --
### Equivalent magnetic circuit --- # Group Exercise-#3 --
### Calculate the airgap flux density for: --- # Group Exercise- #4 --
w a
### Which one creates the most flux density (don't ignore leakage flux)? --- # General PM Machine Structure --
### Surface Mount Permanent Magnet Machine --- # Magnetic Circuit Model
### SMPM magnetic circuit --- # Magnetic Circuit Model
### Series components combined --- # Magnetic Circuit Model
### Leakage ignored --- # Magnetic Circuit Model
### Magnets combined (it is possible to use half-symmetry too) --- # Magnetic Circuit Model
### Steel reluctance ignored (\\(K_r\\) factor added, \\(Kr \gtrapprox 1\\)) --- # Magnetic Circuit Model ## Ideal Airgap Flux Distribution
--- ### Let's see the induced voltage waveform for a full-pitch coil --
--- ### Flux and Induced Voltage in the Coil --
--- ### How about a fractional-pitch coil ? --
--- ### Flux and Induced Voltage in the Fractional-Pitch Coil --
--- ## How about fractional pitch magnets? --
## Reduces the leakage flux between adjacent magnets --- ## Induced voltage in a fractional pitch magnets
--- # Multiple Coils -- ### Nslot= 15, Npoles= 4
--- # Multiple Coils -- ### Nslot= 15, Npoles= 4, 192 degree coil span
--- # Multiple Coils ### Flux Linkage in Single Coil
--- # Multiple Coils ### Induced Voltage in Single Coils
--- # Multiple Coils ### Total Induced Voltage
--- # PMSM vs BLDC -- ## Permanent Magnet Synchronous Motor
--- # PMSM vs BLDC -- ## Brushless DC Motor
### Usually preferred in low cost, small motor --- # PMSM -- ## Sinusoidal Back-EMF
### Sinusoidal back-emf, vector control, precise motion control --- # BLDC -- ## Trapezoidal Back-EMF
### Driven by square wave pulses, small power/low cost applications --- # D-Q Axes Revisited -- ## SM-PMSM -- (Surface Mount Permanent Magnet Synchronous Machine) --
-- ## Ld = Lq for SMPM machines --- # D-Q Axes Revisited -- ## IPM -- (Interior Permanent Magnet Synchronous Machine) --
-- ## Lq > Ld for IPM machines (as \\(\mu_r \approx 1 \\) for PMs) ---