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Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
1
Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
Australian Solar Cooling 2013 Conference
CSIRO, Sydney
11-12 April 2013
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
NEW DEC OPEN CYCLE FOR AIR-CONDITIONING BASED ON FIXED
COOLED ADSORPTION BEDS AND WET HEAT EXCHANGERS
DEIM -Dipartimento di Energia,ingegneria dell’Informazione, e modelli Matematici
Pietro Finocchiaro, Marco Beccali
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
INTRODUCTION
� Thermally driven open cooling cycles are based on a combination of adsorption processes
and evaporative cooling
� In common DEC air handling units, the core components are desiccant wheel, rotating
sensible heat exchanger and humidifiers
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
� System based on simultaneous adsorption and desorption processes
� The use of desiccant rotors implies that condensation heat is rejected
into the processed air and has to be removed by means of the
indirect evaporative process
� The rotating sensible heat exchanger has to carry over two tasks:
� Heat recovery
� Cold production
� Enthalpy difference of the DEC AHU strongly dependent on the
efficiency of sensible heat exchanger and return humidifier
� Leakages and moisture carry over across rotors sealings possible
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
ADSORPTION PROCESS BASED ON DESICCANT ROTORS
� Adsorption process realized by means of desiccant rotors is a quasi – isoenthalpic
transformation
� It presents the disadvantage of causing a temperature increase of the desiccant material
� This phenomena is mostly caused by
the release of adsorption heat due to
water condensation in the desiccant
material and in a lower degree by the
carry-over of heat stored in the
Dehumidification by
desiccant rotor
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
tem
pera
tue
absolute humidity
carry-over of heat stored in the
desiccant material from the
regeneration section to the process
section. (The purge section can limit this
last aspect)
� No enthalpy difference, no cold
production
Outside air
Dehumidification by
cooling coil
Enthalpy difference
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
ADSORPTION PROCESS BASED ON DESICCANT ROTORS
� The higher the
temperature of the
desiccant the lower the
adsorption capacity
� During adsorption in
desiccant rotors, air
50%
60%
70%
80%
90%
100%
RH
[%
] 20 40 60 80
Equilibrium isotherm of
adsorption for silica gel RD
Inlet air
conditions
Air temperature
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
desiccant rotors, air
temperature increases
and relative humidity
strongly decreases
0%
10%
20%
30%
40%
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4
Adsorption bed humidity [kgwater/kgsilica]
Outlet air
conditions
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
ADSORPTION PROCESS BASED ON DESICCANT ROTORS
Furthermore:
� An increase of the desiccant material temperature is
responsible also for higher regeneration temperatures
required
� Regeneration has to be continuously operated if cold
production is requested
� No opportunity to store adsorption capacity into the
desiccant material since they are built to host a relatively
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
desiccant material since they are built to host a relatively
low mass of adsorbent.
� Only option for energy storage is related to the heat
capacity of the regeneration liquid loop
� The use of hot air as regeneration fluid is suitable only
with systems without storage
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
ADSORPTION BED: HEAT AND MASS TRANSFER MECHANISM
� The developed component allows a simultaneous mass transfer between the moist air and
the adsorbent media and heat exchange between the air and the water flowing into the
heat exchanger tubes
� Cooling of the desiccant material during the adsorption process is possible, allowing high
dehumidification performances of the desiccant bed and in general better overall energy
performances of the system
� Water temperatures required can be easily achieved with a cooling tower
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
ADSORPTION BED: HEAT AND MASS TRANSFER MECHANISM
� Very low humidity ratio can be obtained ;
� Adsorption and desorption processes happen in different times;
� Solar energy can be efficiently stored in the desiccant in terms of adsorption capacity which
can be used later when regeneration heat is not available, strongly reducing the necessity
for thermal storage;
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
ADSORPTION PROCESS BASED ON ADSORPTION COOLED BED
� The thermodynamic process causes an enthalpy difference between inlet and outlet air
conditions
� Condensation heat can be rejected
tem
pera
tue
� In general, the temperature of air
exiting the adsorption bed is lower
than the one of incoming air
� Downstream indirect evaporative
cooling process can be operated at
Dehumidification by
desiccant rotor
Enthalpy difference
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
tem
pera
tue
absolute humidity
cooling process can be operated at
lower temperature Outside air
Dehumidification by
cooling coil
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
� During adsorption in
adsorption cooled bed,
air temperature can
sliglty decrease and
relative humidity
ranges from 15% at the 50%
60%
70%
80%
90%
100%
RH
[%
] 20 40 60 80
Equilibrium isotherm of
adsorption for silica gel RD
Inlet air
conditions
Outlet air
ads cooled
bed
ADSORPTION PROCESS BASED ON ADSORPTION COOLED BED
Outlet air
Air temperature
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
ranges from 15% at the
beginning of the
process to 40% at the
end
� Average adsorption
bed humidity at
equilibrium is much
higher than for
desiccant rotors
0%
10%
20%
30%
40%
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4
Adsorption bed humidity [kgwater/kgsilica]
Outlet air
desiccant
rotor
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
DESIGN OF THE COMPONENT
� The total amount of silica gel has to be chosen
according to the dehumidification rate requested,
flow rate to be processed and desired storage of
adsorption capacity
� In order to minimize pressure drops across the bed
the most important issues are:
The adsorption bed should be designed taking into account the following issues:
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
the most important issues are:
� High rate of empty spaces between the
desiccant grains (global porosity of the bed)
� Low air velocity
� Large crossing area, minimum length
� Pressure drop can be similar or lower to the ones
typical for rotors
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
MEASUREMENT TESTS AT UNIPA ON ADSORPTION BEDS
Adsorption bed with cooling
AdsorptionDesorption
60
70
80
20
25
x in x out T in
T out T w out T w in
60
70
80
20
25
x in x out T in T out
Cross section area: 0.24 m 2
Weight of silica gel: 18 kg
Lenght: 13 cm
Flow rate: 210 m3/h
V: 0.26 m/s
DP: 105 Pa
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
0
10
20
30
40
50
0
5
10
15
0:00 1:00 2:00 3:00 4:00 5:00 6:00 7:00 8:00
[°C
]
[g
/kg
]
[h]
0
10
20
30
40
50
0
5
10
15
0:00 1:00 2:00 3:00 4:00 5:00 6:00 7:00 8:00
[°C
]
x [
g/
kg
]
[h]
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
INDIRECT EVAPORATIVE COOLING BASED ON WET PLATE HEAT EXCHANGERS
� cross flow plate heat exchanger operated under
wet conditions
� the surface of secondary flow air channels is
wetted by water spraying, such that the water
evaporates into the cooling air and decreases the
temperature of the heat exchange surface
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
45
50
40
45
50
� Saturation inside the heat exchanger possible
� Temperature of secondary air is close to the
local wet-bulb temperature of the air stream
which increases gradually during the
humidifying process
INDIRECT EVAPORATIVE COOLING: COMPARISON BETWEEN THE SOLUTIONS
� Saturation inside the heat exchanger
not possible
� Secondary air flow passing through
the channels rapidly increases its
temperature
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
10
15
20
25
30
35
40
6 7 8 9 1011121314151617181920
tem
pera
ture
humidity
10
15
20
25
30
35
40
6 7 8 9 1011121314151617181920
tem
pera
ture
humidity
Efficiency: 67% Efficiency: 76%
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
10
12
14
16
65
70
75
80
85
Efficiency T2 in = 25°C Efficiency T2 in = 30°C
Cooling Power T2 in = 25°C Cooling Power T2 in = 30°C
MEASUREMENT TESTS ON WET HEAT EXCHANGERS
87%97%
68%
89%
100%
70%
80%
90%
100%
[Co
oli
ng
po
we
r]
T in HX 1 = 40°C wet operation
T in HX 1 = 40°C dry operation
Efficiency and cooling power Performances vs mass flow rate ratio
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
0
2
4
6
8
10
30
35
40
45
50
55
60
65
30 40 50 60
[kW
]
[%
]
T1 in [°C]
56%
33%
68%
0%
10%
20%
30%
40%
50%
60%
0% 20% 40% 60% 80% 100%
[Co
oli
ng
po
we
r]
Mass flowrate ratio [%]
Flow rate: 1200 m3/h
Flow rate ratio : 1/1
Flow rate of primary:
1200 m3/h
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
DESIGN CONCEPT OF THE NEW DEC CYCLE
Adsorption bed
Dehumidification +
1 st step cooling
Wet heat exchanger
2 nd step coolingOutside
air
Return air
Exausted air
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
� System based on a combination of the proposed solutions for air dehumidification and cooling
� Avoiding or minimizing the use of auxiliary energy source
� System designed for air ventilation, dehumidification and cooling (heating in winter is also
possible)
� Dehumidification and regeneration operated using outside air
� Regeneration carried out using solar air collectors
Exausted air
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
� A portion of the primary air flow rate exiting the wet heat exchanger is drown into the
secondary side
� Electricity consumptions of the system are related to the use of two fans, two pumps and a
cooling tower
DESCRIPTION OF THE NEW DEC CYCLE
� System based on the use of two fixed packed desiccant beds of silica gel operating in a batch
process and cooled by cooling tower, and two wet evaporative heat exchangers connected in
series
� A system of air dumpers provides the commutation between the two adsorption beds in order
to guarantee a continuous dehumidification process
� No auxiliary device included
7
55
60
6540% of supply
air flow rate
50% of supply
air flow rate
100% of air
flow rate
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
12
3
4
7
5
8
6
10
15
20
25
30
35
40
45
50
55
0 2 4 6 8 10 12 14 16 18 20 22 24 26 28 30
Te
mp
era
ture
[°C
]
Humidity ratio [g/kg]
40% of supply
air flow rate
100% of air
flow rate
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
TRNSYS SIMULATIONS
� For the adsorption bed a semi-empirical model (Type 165) partially based on the
approach suggested by Pesaran and Mils was created
� For the simulation of the wet heat exchanger, a modification of the Type 757 was
necessary in order to correctly assess the influence of the variation of the mass flow
rate ratio between the primary and secondary side of the heat exchanger.
� Simulation time step is one minute in order to efficiently describe the dynamic effect
of the desiccant beds
� Commutation time between adsorption and desorption phases is fixed and equal to
0.25 h.
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
0.25 h.
� The system has the configuration described above and is connected to a conditioned
space of about 1200 m3 used as a classroom
� Occupation profile is 150 persons from 8:00 to 13:00, 20 from 13:00 to 15:00 and
100 from 15:00 to 18:00
� The weather data file used is related to the location of Palermo (South Italy) 38°6' N
13°20' E.
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
TRNSYS SIMULATIONS
� AHU flow rate delivered to the conditioned space is 8300 m3/h
� Maximum sensible and latent loads including internal gains, ventilation and infiltration,
are respectively 25 and 51 kW
� Each adsorption bed has a total volume of 0.3 m3 and contains about 115 kg of silica gel
in grains
� A surface of 46 m2 of solar air collectors provides the heat necessary for the
regeneration of the desiccant material
� Solar collector flow rate is 4200 m3/h.
� The maximum electricity consumption for the fans and the pumps is approximately 4.5
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
� The maximum electricity consumption for the fans and the pumps is approximately 4.5
kW when operated at full speed
� The cooling power of the AHU can be varied controlling the speed of the process air fan
� Five days of operation (19th - 23th July) to focus on instantaneous system performances
during typical hot and humid summer days
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
150
200
250
300P
ressu
re d
rop
[P
a]
0.6 - 0.46 m/s
0.5 - 0.46 m/s
0.4 - 0.46 m/s
0.6 - 0.35 m/s
MODEL OF THE ADSORPTION BED: PRESSURE DROPS VERSUS LENGTH, AIR
VELOCITY AND POROSITY
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
0
50
100
150
0.1 0.2 0.3
Pressu
re d
rop
[P
a]
Lenght [m]
0.5 - 0.35 m/s
0.4 - 0.35 m/s
0.6 - 0.28 m/s
0.5 - 0.28 m/s
0.4 - 0.28 m/s
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
ADSORPTION BED VS DESICCANT WHEEL: COMPARISON OF PRESSURE DROPS AT
EQUAL AVERAGE DEHUMIDIFICATION RATE
T in pro 23 °C Area pro 0.1364m2
x in pro 16 °C Flow rate 1250 m3/h
T out pro 55 g/kg Flow mass ratio 2/3
x out pro 5.9 g/kg T rig 80 °C
dx pro 10.1 g/kg Air velocity 2.55 m/s
Dp 188.0 Pa
Desiccant rotor typical operation data
Specific dehumidification capacity: 0.081 kg/h/Pa 0.80
0.6 0.5 0.4 Desiccant rotor
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Adsorption bed
Specific dehumidification capacity: 0.081 kg/h/Pa
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.1 0.2 0.3
[kg
/h/P
a]
Length [m]
Inlet air condition are the same
Adsorption bed cross area: 1 m2
Air velocity: 0.41 m/s
Mass of silica gel: 78 kg for porosity 0.6 and length 0.1 m
350 kg for porosity 0.4 and length 0.3 m
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
TEMPERATURE AND HUMIDITY OF THE AIR IN THE CONDITIONED ROOM
Five days of operation (19th - 23th July)
Building
temperature
Building relative
humidity
Outside humidity
ratio
Outside
temperature
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Flow rate
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
TEMPERATURES IN THE AHU COMPONENTS
Five days of operation (19th - 23th July)
Outlet
temperaure of
solar collectors
Supply
temperature
Range
17-23°C
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Supply wet bulb
temperature
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
COOLING POWER OF THE AHU, SOLAR HEAT PRODUCTION, EFFICIENCY OF
WET HEAT EXCHANGERS
Five days of operation (19th - 23th July)
Cooling power
Wet heat
exchanger
efficiency
Solar heat
Power
Range 60
- 65 %
Range 50 -
90 kW
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
Daily average data
T building [°C] 26.4
RH building [%] 55.2
T supply [°C] 20.7
x supply [g/kg] 10.3
Monthly data - July
SIMULATION RESULTS OF TRNSYS MODEL
3146,
2550,
24%
P Ads Beds P HX 1 P HX 2
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Operation hours [h] 341
Cooling energy delivered by the DEC system [kWh] 10360
Electricity consumed by the DEC system [kWh] 1210
Heat delivered by the solar collectors [kWh] 7450
Electrical COP [-] 8.6
Thermal COP [-] 1,7
Water consumption [m3] 12.1
4985,
47%
3146,
29%
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
CONCLUSIONS
� An innovative solar DEC concept using a combination of fixed cooled adsorption beds
packed with silica gel and two wet heat exchangers was developed and analyzed
� The proposed adsorption bed realizes the simultaneous mass and heat transfer, permitting
to dehumidify and to cool the processed air
� Simulation results have shown high dehumidification potential even in presence of high
humidity values and the opportunity to store the adsorption capacity
� A lower air velocity is needed in comparison to the standard values commonly used for AHU
components
� An accurate design of the desiccant bed can limit pressure drops under 100 Pa
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
� An accurate design of the desiccant bed can limit pressure drops under 100 Pa
� Performance tests have been carried out also on wet plate heat exchangers in several
controlled air conditions, with the aim to assess the efficiency for unbalanced flow rate ratio
� A complete TRNSYS model of the proposed DEC system was created
� Simulation results show that high electrical and thermal COPs can be expected in
comparison to traditional DEC systems
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
PROTOTYPE OF A COMPACT SYSTEM FOR RESIDENTIAL APPLICATION
Collector area: 2 m 2
Flow rate: 500 m 3/h
Max cooling power: 3 kW
Max cooling power to the
Patent pending
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Max cooling power to the cond. room: 1.8kW
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
Thank you for your attention!
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
PERFORMANCE OF THE ADSORPTION BED IN HUMID CLIMATES
20
25
30
35
40
0.015
0.020
0.025
0.030
C]
[kg
/kg
]
Cross section area: 1m 2
Empty space rate: 0.5
Lenght: 0.2 m
Tin: 30°C
x: 22 g/kg
Initial water content of bed: 0.05 kg/kg
M water in : 2000 kg/h
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
0
5
10
15
20
0.000
0.005
0.010
0.015
0.2
5
0.5
0.7
5 1
1.2
5
1.5
1.7
5 2
2.2
5
2.5
2.7
5 3
3.2
5
3.5
3.7
5 4
[°C
]
[kg
/kg
]
[h]
x in x out
T in T out
water in
T water in : 25 °C
DP: 85 Pa
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
PERFORMANCE OF THE ADSORPTION BED IN HUMID CLIMATES
Cross section area: 1m 2
Bed porosity: 0.5
Lenght: 0.2 m
Mass of silica: 194 kg
Tin: 30°C
x: 22 g/kg
Initial water content of bed: 0.05 kg/kg6.0
8.0
10.0
12.0
14.0
70
75
80
85
90
[kW]
[kJ/
kg
K]
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
M water in : 2000 kg/h
T water in : 25 °C
DP: 85 Pa
0.0
2.0
4.0
6.0
50
55
60
65
0
0.2
5
0.5
0.7
5 1
1.2
5
1.5
1.7
5 2
2.2
5
2.5
2.7
5 3
3.2
5
3.5
3.7
5
[kJ/
kg
K]
[h]
h in
h out
Cooling power
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
0.150
0.200
0.250
0.300
[g
/kg
/P
a]
Desiccant rotor
0.5 - 0.3 m
0.5 - 0.2 m
0.5 - 0.1 m
ABSOLUTE HUMIDITY DIFFERENCE FOR UNITARY PRESSURE DROP
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
0.000
0.050
0.100
0.150
0.2
5
0.7
5
1.2
5
1.7
5
2.2
5
2.7
5
3.2
5
3.7
5
[g
/kg
/P
a]
[h]
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
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Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
COMPARISON BETWEEN TRNSYS MODEL AND MEASUREAMENT DATA
Cross section area: 0.25 m 2
Empty space rate: 0.38
Lenght: 0.13 m
Initial water content of bed: 0.05 kg/kg
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
32
Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
Cross section area: 0.25 m 2
Empty space rate: 0.38
Lenght: 0.13 m
Initial water content of bed: 0.05 kg/kg
COMPARISON BETWEEN TRNSYS MODEL AND MEASUREAMENT DATA
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013
Australian Solar Cooling Interest Group (ausSCIG) Conference 2013 www.ausSCIG.org
33
Day 2 – Solar Cooling Conference - 12/04/2013Venue: CSIRO, North Ryde, Sydney
Cross section area: 0.25 m 2
Empty space rate: 0.38
Lenght: 0.13 m
Initial water content of bed: 0.05 kg/kg
COMPARISON BETWEEN TRNSYS MODEL AND MEASUREAMENT DATA
Pietro Finocchiaro – CSIRO, Sydney
12.04.2013