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Power Electronics Passive Components 1

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Page 1: Power Electronics - Lunds tekniska högskola

Power Electronics Passive Components

1

Page 2: Power Electronics - Lunds tekniska högskola

Passive Components

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Page 3: Power Electronics - Lunds tekniska högskola

Types of Passive Components

Resistive

– Heaters, some light sources, ...

Inductive

– Stores energy in magnetic fields

Capacitive

– Stores energy in electric fields

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Page 4: Power Electronics - Lunds tekniska högskola

Inductive Elements

Components

– Inductors

– Transformers

Materials

– Laminated alloys (e.g Silicon-steel, high saturation

level, low frequency range)

– Iron powder composites (lower magnetic saturation

level, low to medium frequency range)

– Ferrites (low saturation level, high frequency range)

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Page 5: Power Electronics - Lunds tekniska högskola

Surahammars M250-35A - laminate

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https://www.emetor.com/edit/materials/sura-m1000-100a/?cat=6&co=10

Page 6: Power Electronics - Lunds tekniska högskola

Soft Magnetic iron Powders Cores

Electric Drives Control 6 https://www.hoganas.com/globalassets/media/sharepoint-

documents/BrochuresanddatasheetsAllDocuments/Inductit_C80.pdf

41 mW/cc =

0.041/(6300/10000) =

0.065 W/kg @ 50 Hz

460 mW/cc =

0.46/(6300/10000) =

0.73 W/kg @ 10 kHz

Page 7: Power Electronics - Lunds tekniska högskola

Ferrite Core material from Mg-Inc

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http://www.mag-inc.com/products/ferrite-cores/p-material

100 mW/cc =

0.1/(4800/10000) = 0.21 W/kg

@ 100 kHz and 100 mT

Page 8: Power Electronics - Lunds tekniska högskola

Inductive Elements - Core Losses

Core losses depend both on frequency and peak flux density

– Usually specified in loss curves (one curve for certain frequencies)

– Also analytical expressions like Steinmetz’s formula:

Steinmetz’s formula includes two loss terms

– Hysteresis loss

– Eddy current loss

Empirical expressions are provided by some core manufacturers

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Page 9: Power Electronics - Lunds tekniska högskola

Inductor Design

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Page 10: Power Electronics - Lunds tekniska högskola

Inductor Core Size Selection

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cucum

cumfew

cumfewcucum

cuwcumfe

mmfe

mm

fe

mm

fe

mmmmagn

kJB

IiLAA

INiLAAkJBN

kAJBAN

iBAN

il

NiAN

iil

NA

iiLiLW

ˆ

ˆ

ˆ2

1ˆ2

1

ˆ2

1

ˆˆ2

1

ˆˆ

2

1

ˆˆ2

1

ˆˆ2

1ˆ2

0

2

0

2

Aw

Page 11: Power Electronics - Lunds tekniska högskola

Core Configurations – Main variants

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EE EI

C Toroidal

Page 12: Power Electronics - Lunds tekniska högskola

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(Guess)

0.4

Page 13: Power Electronics - Lunds tekniska högskola

Flux Fringing factor

”Fringing” leads to:

– Larger air gap area = lower reluctance = higher

flux density in the core

– Losses near the air gap region

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E- and I-cores

Page 15: Power Electronics - Lunds tekniska högskola

FEAN

iL

ˆ

OBS! Different

than from E & I-

cores

VolumeLossSpec

Page 16: Power Electronics - Lunds tekniska högskola

”Mean length per turn”

Thermal flux densities

Emmissivity

Shape

depend

ent

f

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Page 18: Power Electronics - Lunds tekniska högskola

Skin Depth – different metals

Current induction in the core materials forces the flux outside the core

Applies also to the conductor

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Page 19: Power Electronics - Lunds tekniska högskola

Capacitors - Design

Metallized film polypropylene capacitors

– thin plastic film to support the metal layer of the

electrodes.

– the dielectric consists of a polypropylene film.

– to avoid air pockets resulting in a locally high electric field

strength, the polypropylene film should be somewhat

porous to be able to absorb oil.

Wet aluminium electrolytic capacitors

– contain a fluid, the electrolyte, between the aluminium

electrodes.

– the aluminium electrodes are electrically close together,

only separated by the dielectric of the capacitor.

– The dielectric constitutes of a thin aluminum oxide layer

on the positive electrode.

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Page 20: Power Electronics - Lunds tekniska högskola

Capacitors – equivalent circuit

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Page 21: Power Electronics - Lunds tekniska högskola

That’s all folks...

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