splice joint design and analysis john escallier brookhaven national lab bnl - fnal- lbnl - slac us...

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Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

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3 Splice Joint Design overview(2) Splice design affects heat removal to helium Total length and cross sectional area of the NbTi leads within the impregnated structure Current sharing details Splice topology Lead topology and stabilization

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Page 1: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Splice Joint Design and AnalysisJohn Escallier

Brookhaven National Lab

bnl - fnal- lbnl - slacUS LHC Accelerator Research Program

Page 2: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

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Splice Joint Design overview (1)

• Impregnated coil structures have compromised heat paths• Epoxy has limited thermal conductivity• Conductor to epoxy bonds are less thermally

conductive than the epoxy or the metals• TCE mismatches fracture epoxy to metal bonds

• Splice joints generate heat from IR loss• Splice design affects generated heat

• Total overlap area• Solder thickness• Joint topology

Page 3: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

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Splice Joint Design overview(2)

• Splice design affects heat removal to helium• Total length and cross sectional area of the NbTi

leads within the impregnated structure• Current sharing details

• Splice topology• Lead topology and stabilization

Page 4: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Full heat flux pathway

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Heat to helium

Heat to coils

Peak source temperature

Spread to turns

Spread to adjacent coil

Dissipation sourceSolder

(green)Niobium Titanium

(orange)

Niobium3 Tin(maroon)

Page 5: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Steady state condition

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Page 6: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Splice joint temperature profile at 11 kAmps

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Assumptions:11 Kiloamp current (input variable)

Joint resistances of 1 nano-ohm (input variable)Uniform joint cross section

NbTi cable effective thermal conductivity 70% room temperature copper (input variable)

No thermal path provided by epoxyLiquid helium temperature of 4.5 kelvin (input variable)

Linear material properties in the 4 to 10K range (equations may be used)

Page 7: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Impact of effective joint resistance on final temperature at 11 kAmps

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Page 8: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Overview of possible splice geometries

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Page 9: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Interconnect type A

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Soldering the two leads will current share and reduce

dissipation by 20 percent

(5.3 Kelvin if the leads are soldered together their length)

Page 10: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Interconnect type B

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5.3 Kelvin final temperature

Page 11: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

Interconnect type C

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4.9 Kelvin final temperature

Page 12: Splice Joint Design and Analysis John Escallier Brookhaven National Lab bnl - fnal- lbnl - slac US LHC Accelerator Research Program

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Splice Joint Summary

• Vacuum impregnation:• removes direct helium contact cooling of all

conductors and connections•creates higher temperatures internally given

internal dissipations• Splice design requires configuring conductor

layers in the splice for reduced dissipation• Splice design needs to provide adequate thermal

conductive paths to helium for generated heat• I squared R dissipated heat