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Mathematical and Mathematical and Statistical Analysis Statistical Analysis
of Heat Pipe Designof Heat Pipe Design Sandy DeSousaSandy DeSousa Cuong DongCuong Dong
Sergio de OrnelasSergio de Ornelas Michelle FerneliusMichelle Fernelius
Marian HoferMarian Hofer Tracy HolsclawTracy Holsclaw
Adam JennisonAdam Jennison Diem MaiDiem Mai
Kim NinhKim Ninh Misako van der PoelMisako van der Poel
All heat pipes and data presented today are purely fictional. Any similarity with any heat pipe, functioning or not, is purely coincidental.
Requirements for CoolingRequirements for Cooling
Solid metal rods lose Solid metal rods lose too much heat to the too much heat to the environmentenvironment
Cannot use a Cannot use a powered cooling powered cooling system, too much system, too much power consumption power consumption caused the problemcaused the problem
Heat
Transfer of HeatTransfer of Heat
Heat PipeHeat Sink
Processor
Heat Added Heat Released
*Drawing is not to scale.
Evaporation Condensation
Heat Absorbed
Heat Absorbed Heat Released
Heat Released
Heat Transfer within Heat Transfer within a Heat Pipea Heat Pipe
*Drawing is not to scale.
Wick Structure
Wick Structure
Container
Container
MEDIUMMEDIUM
MELTING MELTING PT. (° C ) PT. (° C )
BOILING PT. AT BOILING PT. AT ATM. PRESSURE ATM. PRESSURE
(° C) (° C)
USEFUL USEFUL RANGERANGE
(° C)(° C)
HeliumHelium
AmmoniaAmmonia
WaterWater
Silver Silver
- 271- 271
- 78- 78
00
960960
- 261- 261
- 33- 33
100100
22122212
-271 to -269-271 to -269
-60 to 100-60 to 100
30 to 20030 to 200
1800 to 2300 1800 to 2300
Created by carving out grooves on the interior Created by carving out grooves on the interior core of the Heat Pipe. core of the Heat Pipe.
TermTerm P-valueP-value
ConstantConstant 0.0000.000
PowderSizePowderSize 0.0000.000
WickThicknessWickThickness 0.4670.467
LiquidChargeLiquidCharge 0.0000.000
PowderSize*WickThicknessPowderSize*WickThickness 0.0000.000
PowderSize*LiquidChargePowderSize*LiquidCharge 0.0000.000
WickThickness*LiquidChargeWickThickness*LiquidCharge 0.0210.021
PowderSize*WickThickness*LiquidChargePowderSize*WickThickness*LiquidCharge 0.0050.005
Individual 95% CIs For Mean Individual 95% CIs For Mean HP Mean --+---------+---------+---------+-----HP Mean --+---------+---------+---------+----- 5 1.01 (-*-)5 1.01 (-*-) 13 1.06 (-*-)13 1.06 (-*-) 17 1.09 (-*-)17 1.09 (-*-) 9 1.12 (-*-)9 1.12 (-*-) 19 1.22 (-*-)19 1.22 (-*-) 15 1.40 (-*-)15 1.40 (-*-) 11 1.61 (-*-)11 1.61 (-*-) 7 1.62 (-*-)7 1.62 (-*-) --+---------+---------+---------+-------+---------+---------+---------+----- 1.00 1.20 1.40 1.601.00 1.20 1.40 1.60
The minimum occurs at:
Powder size = 77.2
Wick thickness = 0.65
Liquid charge = 138
Ө = 0.5988
Response SurfaceResponse Surface
39% Improvement
θ
Does variability in the manufacturing process Does variability in the manufacturing process
affect our analysis?affect our analysis? There are 3 heat pipes of “identical” constructionThere are 3 heat pipes of “identical” construction
170 mm
Evaporator 65 mm
Adiabatic
30 mm Condenser 75 mm
Wick thickness .75 mm
Copper thickness .25 mm
Axis
p(T) is the saturated vapor pressure at T.p(T) is the saturated vapor pressure at T. Viscosity and density of vapor change with Viscosity and density of vapor change with
temperature.temperature.
No slipu = 0
Axis
Viscosity of water change with temperature.Viscosity of water change with temperature. K (permeability of wick structure) depends of the K (permeability of wick structure) depends of the
porosity and size of sphere.porosity and size of sphere.
Slip condition