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Energies 2017,10, 315
whereB1andB2aretherightandleftmagneticfields, respectively,asshowninFigure9.Whenviewed
fromthey-axisdirection, fromthedirectionthe loopof thesensorcoil is facing,BS canbeexpressed in
vector formasfollows:
Bsy=B
1
y+B
2
y=− μ0I1
2πr1 sinθ1+ μ0I2
2πr2 sinθ2 (8)
In(8), I1, I2, θ1andθ2arethecurrentflowandtheangleneededtogenerateB1andB2, respectively.
It shouldbenoted that I1 and I2 have the samemagnitudesbutflow inoppositedirections. μ0 is
the free-spacepermeability and r1, r2 are the referencepoint distances ofB1 andB2, respectively.
InFigure9a, themagneticfieldsensedbythesensorcoil isnearzerobecauseB1andB2 canceleach
otherout.As thesensorcoilmoves towards the left, as showninFigure9b, thesensorcoil is relatively
moreexposedto theB2magneticfield, thus themagnitudeofB2willbemoredominant thanB1. The
oppositephenomenonwilloccurwhenthesensorcoilmoves towards theright,where themagnitude
ofB1willbemoredominant thanB2, as showninFigure9c.
The inducedvoltage in thesensorcoil,Vse, canbeexpressedas follows:
Vse=−dΦdt =− dBSA
dt (9)
where theequation isbasedonFaraday’s law.Φ, tandA represent themagneticflux, time,andcross
sectionalareaof thesensorcoil, respectively.Whenthe loadcoil ismisalignedto the leftor right, the
phaseangledifferencebetweenthesensorcoilwill alwayshavea±90degreedifference, respectively.
Thephasedifferencewillonlychangewhenthe loadcoil is shifted fromtheright region to the left
region,orviceversa.Under theseconditions, thedifference inphasewhenthecoil ismisalignedto the
left (showninFigure9b)andright (showninFigure9c)willbearound180degrees.
Verificationof theACASSensorCoilUnit throughSimulation
3-DEMsimulationswereconductedtoverify that theplacementof thesensorcoildoesnothave
much influenceon thepower transferbetween the source coil and loadcoil, andalso toverify the
concept shown inFigure9. The sensor coilwasadded to the simulationmodel shown inFigure4
tomatch theconfigurationshowninFigure8. Thesensor coilparameterswereas listed inTable1.
Figures10and11showcomparisonsof the inducedvoltageandmagneticfluxdensityof the loadcoil
withthesensorcoil, andtheloadcoilwithout thesensorcoil, respectively,whenalateralmisalignment
occurs from−50cmto50cm.
Figure10. Simulationresults showing inducedvoltagevs. lateralmisalignment.Acomparisonof load
coilswithandwithout thesensorcoil.
BasedonFigure10, the twooutputwaveformsarenearly identical, andthemagneticfluxdensity
comparison inFigure11showsthat theexistenceof thesensorcoilunit createsalmostno interference
with themagneticflowbetweenthe loadcoilandsensorcoil. Thisverifies that theplacementof the
sensorcoilhas littleeffectontheperformanceof theoverallWPTsystem.
332
Emerging Technologies for Electric and Hybrid Vehicles
- Title
- Emerging Technologies for Electric and Hybrid Vehicles
- Editor
- MDPI
- Location
- Basel
- Date
- 2017
- Language
- English
- License
- CC BY-NC-ND 4.0
- ISBN
- 978-3-03897-191-7
- Size
- 17.0 x 24.4 cm
- Pages
- 376
- Keywords
- electric vehicle, plug-in hybrid electric vehicle (PHEV), energy sources, energy management strategy, energy-storage system, charging technologies, control algorithms, battery, operating scenario, wireless power transfer (WPT)
- Category
- Technik