Arsene Noume Carmen Vasile Amadou CoulibalyDevelopment of an efficient air-conditioning and heating...
Transcript of Arsene Noume Carmen Vasile Amadou CoulibalyDevelopment of an efficient air-conditioning and heating...
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Arsene Noume
Carmen Vasile
Amadou Coulibaly
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Development of an efficient air-conditioning and heating
system based on Magneto-Caloric heat pump
New system architecture to fulfill the thermal comfort
and energy requirements of a FEV
Heating power: 5 kW
Cooling power: 3 kW
Temperature span:-7°C,+50°C
COP ≥ 3
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Based on Magneto-Caloric Effect (MCE)
MCE: temperature changing of a magneto-caloric material
exposed to a changing magnetic field
Active Magnetic Regenerator (AMR)
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Active Magnetic Regenerator cycle(AMR cycle)
(1)
Adiabatic magnetization
(2)
Isofield cooling
(Maximal magnetic field)
(3)
Adiabatic demagnetization
(4)
Isofield heating
(Minimal magnetic field)
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Model of fluid flow and heat transfer in Minichannel
∇ ∙ 𝑢 = 0
𝜌𝑓 𝑢 ∙ ∇ 𝑢 = −∇𝑝+ 𝜇𝑓∇2𝑢
𝜌𝑓𝐶𝑝 ,𝑓 𝑢 ∙ ∇𝑇𝑓 = 𝑘𝑓∇2𝑇𝑓
𝑘𝑠∇2𝑇𝑠 + 𝑄0 = 0
ℎ =𝑞𝑤𝑎𝑙𝑙
𝑇𝑤𝑎𝑙𝑙 − 𝑇𝑓
Mass conservation equation
Momentum equation
Energy equation for fluid domain
Energy equation for solid domain
Equation for heat transfer coefficient
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Physical model of AMR cycle
𝜌𝑓𝐶𝑝 ,𝑓 𝜕𝑇𝑓
𝜕𝑡+ 𝑢 ∙ ∇ 𝑇𝑓 = ∇ ∙ 𝑘𝑓∇𝑇𝑓 − 𝑄 𝑇𝑇
𝜌𝑠𝐶𝑝 ,𝑠𝜕𝑇𝑠𝜕𝑡
= ∇ ∙ 𝑘𝑠∇𝑇𝑠 + 𝑄 𝑀𝐴𝐺 + 𝑄 𝑇𝑇
𝑄 𝑀𝐶𝐸 = 𝜌𝑠𝐶𝑃,𝑠 𝜕𝑇𝑎𝑑𝜕𝐻
𝑑𝐻
𝑑𝑡+𝜕𝑇𝑎𝑑𝜕𝑇𝑠
𝑑𝑇𝑠𝑑𝑡
𝑄 𝑇𝑇 = ℎ𝛽 𝑇𝑠 − 𝑇𝑓 𝐼𝑛𝑡 :𝑓/𝑠
Energy equation for fluid
Energy equation for solid
Equation of MCE source term
Equation of heat transfer between
fluid and solid as source term
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Interpolation of Cp and ∆Tad of Gadolinium
Variation of ∆Tad with temperature, for
0 ≤ µ0H ≤ 2 T
Variation of Cp with temperature, for
0 ≤ µ0H ≤ 2 T
0 0
0
, ,,
Gd Gd
MCE Gd Gd
Tad T H t dt Tad T H tQ Cp T H t
dt
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x [mm]
Heat transfer coefficient
8000
10000
12000
14000
16000
18000
20000
0 0.005 0.01 0.015 0.02
Co
eff
cie
nt
d'é
chan
ge c
on
vect
if [
Wm
-2K
-1]
Longueur du canal [m]
h en fonction de la longuer de canal: comparaison des modèles numériques et des modèles empiriques
Comsol
Matlab
Shah et London
Churchill et Usagi
h [
W.m
-2K
-1]
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Temperature field
solid
fluid
Hot end and cold end temperatures of the cycle
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Contributions
A different and acurate approach to
calculate de QMCE
An accurate determination of heat transfer
coefficient
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Implementation of QMCE
Requirement of high quantity of memory
Analyse the surface rugosity influence on the fluid flow and
heat transfer in microchannels.
Analyse the influence of the dimensions of the system (plate
thickness, channel height) on the heat transfer quantities.
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THANKYOU!
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0
50
100
150
200
250
300
350
0 200 400 600
Cp
[J/(
kg K
)]
T [K]
µ0H = 0 [T]
W-D-S (TD = 169 K)
Expérimental
W-D-S (TD = 220 K)
0
50
100
150
200
250
300
0 200 400 600
Cp
[J/(
kg K
)]
T [K]
μ0H = 1 [T]
W-D-S (TD = 169 K)
Experimental
W-D-S (TD = 220 K)