hapl meeting, madison, wi (september, 24-25, 2003)
DESCRIPTION
Experimental and Numerical Study of Mist Cooling for the Electra Hibachi V.Novak, D.Sadowski, S.Shin, K.Schoonover, and S. Abdel-Khalik. HAPL meeting, Madison, WI (September, 24-25, 2003). G. W. Woodruff School of Mechanical Engineering Atlanta, GA 30332 – 0405 USA. Diode (vacuum). - PowerPoint PPT PresentationTRANSCRIPT
Experimental and Numerical Study of Mist Cooling for the
Electra HibachiV.Novak, D.Sadowski, S.Shin, K.Schoonover,
and S. Abdel-Khalik
HAPL meeting, Madison, WI (September, 24-25, 2003)
G. W. Woodruff School ofMechanical Engineering
Atlanta, GA 30332–0405 USA
2
Objectives
• Experimentally examine effectiveness of gas/liquid mist as a means of cooling the Electra Hibachi Foils
• Quantify effect of various operating parameters on mist cooling effectiveness for prototypical Hibachi geometry (gas/liquid combination, gas velocity, liquid mass fraction, droplet size)
• Develop a validated mechanistic model to predict Hibachi foils’ thermal response under prototypical pulsed operating conditions
Laser Gas1.3-2.0 atm
(Kr+F2)flow at 4 m/s
Diode(vacuum)
E-beam
HibachiRibs
HibachiFoils
PressureFoil
Water Layers
VACUUM
E-beam
LASERGAS
EMITTER
He(or Air)/Water mix
Anode Foil
3
Experimental Setup
4
Air-Assisted Nozzle
Experimental ResultsAir/Water Mist Cooling – Rectangluar Channel (24 cm)
Water inlet mass fraction [%] Water inlet mass fraction [%]
Axial distance [cm] Air-assisted nozzle inlet pressure [psi]
Ave
rage
hea
t tra
nsfe
r co
effi
cien
t [W
/m2
K]
Loc
al h
eat t
rans
fer
coef
fici
ent [
W/m
2K
]
Ave
rage
hea
t tra
nsfe
r co
effi
cien
t [W
/m2
K]
Ave
rage
hea
t tra
nsfe
r co
effi
cien
t [W
/m2
K]
Ave
rage
enh
ance
men
t rat
io [
h/h
dry
air]
water inlet mass fraction [%]
Ultrasonic Nozzle
Max Twall=80-90oC
15m/s
10m/s
5m/s
15m/s10m/s
5m/s
15m/s,dry air
15m/s,15%
15m/s,10%
15m/s,5%
15m/s
10m/s
5m/s
Optimization of atomizing air mass fraction
(10m/s air,10% water)
5
Numerical Simulation steady state experiment (Air/Water)
4 cm
60 cm
2 cm
Heating (Qw)
Heating (Qw)
foils(Hastelloy-X=0.25 mm)
insulated side wall
6 cm
Air/Water Mist Flow [100% Saturation]
(Tin=20 oC, 1 atm, rp=30 m)Coolant
TemperatureFront SurfaceTemperature
Back SurfaceTemperature
Coolant Distribution Particle Distribution
ParticleTemperature
6
Numerical Simulation steady state experiment (Air/Water)
Coolant Exit TemperatureCoolant Bulk Temperature Pressure
T
[K]
P [
kPa]
z [cm] z [cm]
Solid line : Coolant bulk temperature Dash dot line : Wall temperature
Wall and Coolant Temperature Distribution
dry air (15m/s, Qw=250W)
0 % water4 % water 5 % water 10 % water15 % water
15m/s Air
Qw=250W
rp=30 m
Heat transfer coefficient at the wall Wall film thickness
7
dry Helium (30m/s, Qw=250W)
Numerical Simulation steady state experiment (Helium/Water)
Coolant Exit Temperature
T [
K] Solid line : Coolant bulk temperature
Dash dot line : Wall temperature
Wall and Coolant Temperature Distribution
Heat transfer coefficient at the wall30m/s Helium
Qw=250W
rp=30 m
0 % water 16.7 % water 33.5 % water50.2 % water
Coolant Bulk Temperature Pressure
T
[K]
P [
kPa]
z [cm] z [cm]
8
Numerical Simulation pulsed heating (10Hz)
time [sec]
Q [
W/c
m3]
0.1 s
587250 W/cm3
pulse start at 4.0 s0
0.1ms
30 cm
2 cm
Heating
Heating
foils (Titanium, =0.025mm)
insulated side wall
4 cm
Air/Water Mist Flow [0% Saturation]
(15m/s Air, 10% Water Tin=20 oC, 1 atm, rp=30m)
Coolant TemperatureFront Surface
TemperatureBack SurfaceTemperature
Coolant Distribution Particle Distribution
ParticleTemperature
9
Numerical Simulation pulsed heating (10Hz)
Coolant Exit Temperature
Dry Air
Air/Water(15m/s, 15%)
Maximum Temperature at the wall
Dry Air
Air/Water(15m/s, 15%)
10
Numerical Simulation pulsed heating (10Hz)
Coolant Temperature Distribution Surface Temperature Distribution Heat Transfer Coefficient Distribution
Dry Air
(15m/s,15%)
A B C t [sec]
A : just before pulseB : just after pulseC : one pulse later
Air/Water
11
Conclusions
•Mist cooling provides the means to effectively cool the Electra Hibachi within specified constraints on cooling system power consumption, foil max temperature, and temperature gradient Heat transfer coefficient can be significantly increased especially for
prototypical transient condition
•A validated mechanistic model to predict the foils’ thermal response under prototypical conditions has been developed
12
Future Efforts
•Examine effect of liquid film formation on e-beam transmission efficiency
•Examine system performance for other gas/liquid combinations
•Construct and test a multi-channel test module under prototypical conditions