Towards a Finite Element Calculation of A ti l A lit d i HID Lf … · 2009-12-01 · Towards a...

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Towards a Finite Element Calculation fA ti lA lit d i HID L of Acoustical Amplitudes in HID Lamps Bernd Baumann 1 , Marcus Wolff 1 , John Hirsch 2 , Piet Antonis 2 , Sounil Bhosle 3 and Ricardo Valdivia Barrientos 4 1) Hamburg University of Applied Sciences, Germany 2) Philips Lighting, Eindhoven, The Netherlands 3) Université de Toulouse and CNRS LAPLACE, Toulouse, France 4) National Institute of Nuclear Research, Salazar, Ocoyoacac, Mexico www.berndbaumann.de | Milan, October 2009 | page 1 Presented at the COMSOL Conference 2009 Milan

Transcript of Towards a Finite Element Calculation of A ti l A lit d i HID Lf … · 2009-12-01 · Towards a...

Page 1: Towards a Finite Element Calculation of A ti l A lit d i HID Lf … · 2009-12-01 · Towards a Finite Element Calculation of A ti l A lit d i HID Lf Acoustical Amplitudes in HID

Towards a Finite Element Calculationf A ti l A lit d i HID Lof Acoustical Amplitudes in HID Lamps

Bernd Baumann1, Marcus Wolff1, John Hirsch2, Piet Antonis2,, , , ,Sounil Bhosle3 and Ricardo Valdivia Barrientos4

1) Hamburg University of Applied Sciences, Germany2) Philips Lighting, Eindhoven, The Netherlands3) Université de Toulouse and CNRS LAPLACE, Toulouse, France4) National Institute of Nuclear Research, Salazar, Ocoyoacac, Mexico

www.berndbaumann.de | Milan, October 2009 | page 1

Presented at the COMSOL Conference 2009 Milan

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Energy Consumption

Industrial production Transportation Transportation Heating and cooling Lightingg g …

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High Intensity Discharge (HID) Lamp

Arc tube / burner– Wall: Quartz or ceramicsWall: Quartz or ceramics– Filling: Mercury– Additives: Metal halides etc

Electrodes Electrodes– Tungsten

Discharge arcg– Light source– Temperature 5000 – 6000 K

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AC Operation

Advantages:– Avoids demixingAvoids demixing– Avoids electrode errosion

Acoustic resonance problem:Fli k i– Flickering

– Reduction of lamp‘s lifetime– Lamp destruction

Counteraction:– Electronical measures– Lamp design– Lamp design

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Objective and Scope

Numerical calculation of acoustic amplitudesin HID lampsp

Enhancement of unterstanding of acousticalresonance problemSi lifi i Simplifications:– No inclusion of plasma dynamics– Simplified geometryp g y– 2 dimensional axisymmetric FE model

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Temperature Profile

(Sutherland’s law)

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Gaussian Power Density

Cylinder axis

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Inhomogenous Helmholtz Equation

Ideal gas law

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Solution

Eigenmodes

Boundary conditions: Burner walls sound hardBoundary conditions: Burner walls sound hard

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Amplitudes

Excitation amplitude:

Loss factor

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Surface Loss: Shear Stress

fluid

P dtl‘ b d l

ceramics

Prandtl‘s boundary layer

ceramics

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Surface Loss: Shear Stress

fluid

P dtl‘ b d l

ceramics

Prandtl‘s boundary layer

ceramics

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Surface Loss: Thermal Conduction

adiabatic region

region of transistiong

isothermal regionCeramics isothermal region ???isothermal regionCeramics isothermal region ???

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Surface Loss: Thermal Conduction

adiabatic region

region of transistiong

isothermal regionCeramics isothermal region ???isothermal regionCeramics isothermal region ???

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Surface Loss: Thermal Conduction

Metallic wall:

Ceramic wall:

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Volume Loss: Thermal Conduction

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Volume Loss: Shear Stress

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Volume Loss: Shear Stress

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Volume Loss

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Volume Loss

C iti l d iCritical damping:

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Measuring Points

Cylinder axisCylinder axis

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Response Function and Excitation Amplitude

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Response Function and Excitation Amplitude

All l lit dAll large amplitudescorrespond to radial modes!

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Radial Modes

P d itPower density

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Nonradial Modes

P d itPower density

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Nonradial Modes

P d itPower density

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Nonradial Modes

P d itPower density

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Summary, Conclusions and Prospect

Simplified model for calculation ofacoustical resonances in HID lampsp

Finding: Excitation amplitudes are the key for controlling acoustical resonancesN Next steps– Inclusion of plasma dynamics– Extension to 3d model– Optimization of burner geometry

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Molto grazie!

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