High Bs Ferrite Material for high power applications High Bs...Alex Goldman: modern ferrite...
Transcript of High Bs Ferrite Material for high power applications High Bs...Alex Goldman: modern ferrite...
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High Bs Ferrite Material for high power applications
JC SunBs&T Frankfurt am Main GmbH
19. March 2019APEC 2019 Anaheim (CA)
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physicist & engineer
make and design ferrite 3Cx and 3Fx
sales amorphous metals 2605/2714/2705
marketing nanocrystalline 500F components
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JC and his...
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content
• Introduction Bs&T
• Demand on ferrite material development
• Need for high power application
• High Bs material for high power and high frequency application
• Material design route (high Bs and low loss)
• Conclusion
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Bs & T Analyzer
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Sinus Magnetization AC Pulse Magnetizationhigh excitation low excitation fast transit of magnetic state
IEC 62044-3 IEC 62044-2 dB/dt
loss, µa driven by B mode IEC 60367-1 Annex G
Bpeak, loop driven by H mode
DC superposition
BsT-Pro BsT-Pulse
loss map (f, B, T, HDC) µrev differential and amplitude L,
major, and biased minor loop energetic L, power loss i.e. Q factor
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Bs & T Analyzer
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Square Wave
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Demand on ferrite material
• Driving forces for development of ferrite material
information and communication technologyenergy digitalization
• High power and power density application require new materials outside of the conventional power ferrite material performance factor map
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Soft magnetic behavior
• „Good“ soft magnetic behavior:large magnetization changes as a result of very smallapplied magnetic fields ~ high permeable material
easy rotation of magnetization vectoreasy motion of domain wallhigh versatility
• „Ideal“ soft magnetic material:magnetically isotropic and structurally homogeneous, no crystallographic easy axis, no defects, no grainboundary, no internal stress, no magnetostriction
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Design consideration of softmagnetic materials
• Intrinsic material properties, depend only on chemical composition (unaffected by the microstructure), are:Tc, Bs and crystalline anisotropy K1, λsselective choice of the chemical composition
• Structure sensitive properties are:Hc, Br and permeability µproper processing route
The most important microstructural parameters are: grain size, crystallographic texture, lattice defects volume fraction, as well asthe size and chemical nature of non-magnetic inclusion and internal stresses
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Performance factor 300 mW/cm3 @ 100°C material
map
nanocrystalline
Alex Goldman: modern ferrite technology
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Component design consideration for material choice
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Correlation magnetic component, core and material
component core material
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High power application for high voltage
• P = U I
• High U; U = dB/dt
• Large I; low permeable cores(powdered, gapped, stress annealed artificial processed)
• Need for magnetic component is high flux linkage, corresponding to large accessible working flux density
• High Bs material
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How to achieve the highest
Bs MnZnFerrite material ?
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State of art methodology D9BAchievement !
600 K
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High power density application for high frequency
• High switching frequency requires high resonance frequencySnoek’s fR ~ Ms / µ
Ms/Bs should be as high as possible (coherent), at same time the µ should be as low as possible
• Key issue is heat dissipation @ MHz
how much do we know about material properties likeresistivity and permittivity ?
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Example: resistivity for high frequency
the dc resistivity roughly scales as the resistivity of the grain boundaryRg: V2O5, Nb2O5 Rb: SnO2 , SiO2, CaO, TiO2, CoOCb: Ta2O5
IEEE TRANSACTIONS ON MAGNETICS, VOL. 50, NO. 1, JANUARY 2014
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High frequency ω→++Rg
Low frequency ω→0Rg + Rb
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Loss at (very) high frequency (MHz)
F.Fiorillo INRIM 2010
VNA
fluxmetric
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Chemistry dopants for high resistivity
Resistivity on grain 3F3
Resistivity on boundary 3F4
Number of publication ICF 6 /7 about dopants are available
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https://www.google.de/url?sa=i&rct=j&q=&esrc=s&source=images&cd=&cad=rja&uact=8&ved=2ahUKEwju2PXhpOHeAhXJsaQKHWRRDqwQjRx6BAgBEAU&url=http://jugendamt-bonn-erfahrungsbericht.de/wett-strategien/kicktipp-lizas-welt.html&psig=AOvVaw1o7WjZ29OTN4DnZISDDj19&ust=1542745378195643
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High Bs ferrite material for future application
• Either high power, or high frequency ferrite material needs highest possible Bs, which is limited by physics (antiferrimagnetism)
• Highest Bs ferrite material for high voltage application. The benefit in combination with the largest possible size as monolith in favor of high power magnetic component design (core height 5 inch, and length of 8 inch)*, commercially available
• Highest Bs ferrite material is essential for application of the highest possible resonance frequency: trade-off MnZnFerrite vs. NiZnFerrite
• High resistivity with comprehensive investigation with number of dopants at expense of Bs has been studied since decades, the chemical composition is just only one consideration, the morphological optimization is process related for loss performance
• Resistivity @ applied frequency and operation temperature have to be firstly specified as material properties
* IEEE September 2018Recent Ferrite material development for high power application
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Requirements on material are: high Bs and low loss (large DC biased high frequency rippled AC loss)
• more capability 20% than reference ferrite material to handle more power
• Curie temperature over 600 K is more thermal stable than reference ferrite material
• Less permeability, less air gap length, less fringing, less component loss than reference design
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Targeted application: buck
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Example: more power handling capability and better
thermal stable compared with reference design
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Conclusion
• MnZnFerrite material for high voltage WBG power semiconductor is commercial available, its power magnetic component can be charaterized by BsT-pulse(damped oscillation) funded by EU H2020 and VDE DIN-Connect, dB/dt provides useful assignments of magnetization inductance and current
• MnZnFerrite for high frequency application is still vague, and under development, the most critical part is experimental approval by suitable measuring technique due to problem with thermal inequilibrium, BsT-SQ can be a help (GaN bridge loss tester)
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Annex 1 measuring data for simulation
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BsT-Pro 2016BsT-SQ 2018
BsT-Pulse 2017
BsT-ProBsT-SQ
BsT-Pulse
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Annex 2 BsT-Pulse
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1. assignment inductance vs. current NOT unique
2. Voltage decay pending on DUT
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Annex 3 BsT-SQ with Herbert Curve
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mW
µs
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Annex 4 Diverse D.U.T.s
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Power ferrite Fe amorphous
metal alloyed powder “HF” ferrite