Accepted Manuscript Absorption solar cooling systems using optimal driving temperatures Antonio Lecuona, Rubén Ventas, Ciro Vereda, Ricardo López PII:
S1359-4311(15)00016-2
DOI:
10.1016/j.applthermaleng.2014.10.097
Reference:
ATE 6280
To appear in:
Applied Thermal Engineering
Received Date: 24 June 2014 Revised Date:
22 September 2014
Accepted Date: 26 October 2014
Please cite this article as: A. Lecuona, R. Ventas, C. Vereda, R. López, Absorption solar cooling systems using optimal driving temperatures, Applied Thermal Engineering (2015), doi: 10.1016/ j.applthermaleng.2014.10.097. This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.
ACCEPTED MANUSCRIPT 2 3 4 5 6 7 8 9
Absorption solar cooling systems using optimal driving temperatures Antonio Lecuona*, Rubén Ventas, Ciro Vereda, Ricardo López. Departamento de Ingeniería Térmica y de Fluidos, Universidad Carlos III de Madrid, Avda. Universidad 30, 28911 Leganés, Madrid, Spain. * Tel: (34) 916249475; Fax: (34) 91 624 9430; e-mail:
[email protected]
RI PT
1
10 11 12 13 14
Abstract
15
along a day. The chillers compared use single effect cycles working with NH3/LiNO3,
16
either conventional or hybridised by incorporating a low pressure booster compressor.
17
Their performances are compared with a H2O/LiBr single effect absorption chiller as
18
part of the same solar system. The results of a detailed thermodynamic cycle for the
19
absorption chillers allow synthesizing them in a modified characteristic temperature
20
difference model. The day accumulated solar cold production is determined using this
21
optimum temperature during two sunny days in mid-July and mid-September, located in
22
Madrid, Spain. The work shows the influences of operational variables and a striking
23
result: selection of a time-constant temperature during all the day does not necessarily
24
imply a substantial loss, being the temperature chosen a key parameter. The results
25
indicate that the NH3/LiNO3 option with no boosting offers a smaller production above-
26
zero Celsius degrees temperatures, but does not require higher hot water driving
27
temperatures than H2O/LiBr. The boosted cycle offers superior performance. Some
28
operational details are discussed.
AC C
EP
TE D
M AN U
SC
The optimum instantaneous driving temperature of a solar cooling facility is determined
29
1
ACCEPTED MANUSCRIPT 30
Keywords: solar cooling, optimum hot water temperature, hybrid cycle, chillers,
31
NH3/LiNO3, H2O/LiBr.
32
Nomenclature
33 a
Absorber; Constant
35
As
Collector area, m2
36
b
Constant
37
COP Coefficient of performance
38
COPe Electrical coefficient of performance
39 40 41
COPM Asymptotic value for COP when ∆∆t → ∞. c
Condenser
42
e
Evaporator
43
g
Generator
44
GT
Solar intensity, tilted, W/m2
45
h
Specific enthalpy, external fluid, J kg-1
46
H
Specific enthalpy, internal fluid, J kg-1
47
m&
Mass flow rate, external fluid, kg/s
48
M&
Mass flow rate, internal fluid, kg/s
49
P
50
pr
51
Q
52
Q&
53
SCOP Solar coefficient of performance
54
SE
Single-effect
55
she
Solution heat exchanger
AC C
EP
TE D
M AN U
SC
RI PT
34
Pressure, Pa
Pressure ratio of booster compressor
Daily solar cold production, J/m2
Heat power, W
2
ACCEPTED MANUSCRIPT t
Averaged external fluid temperature between inlet and outlet, ºC
57
t’e
Equivalent external fluid temperature averaged between inlet and outlet, ºC
58
tg,op
Optimum external generator temperature averaged between inlet and outlet, ºC
59
tg,0
Activation external generator temperature averaged between inlet and outlet, ºC
60
T
Averaged internal fluid temperature between inlet and outlet, ºC
61
T’e
Equivalent internal fluid temperature averaged between inlet and outlet, ºC
62
UA
Heat exchanger thermal conductivity, W/ºC
63
Mechanical power to the booster compressor W
SC
RI PT
56
64 Greek
66
∆∆t
Characteristic temperature difference, ºC
67
∆Tml
Mean logarithmic temperature difference, ºC
68
ε
Efficiency of heat exchanger in the solar facility
69
η
Isentropic efficiency of the compressor
TE D
M AN U
65
70 Subscripts
72
a
Absorber
73
ac
Absorber-Condenser
74
atm
Atmospheric
75
c
Condenser
76
e
77
g
Generator
78
i
Inlet
79
o
Outlet
80
r
Solution or refrigerant, internal fluid of the absorption chiller
AC C
EP
71
Evaporator
3
ACCEPTED MANUSCRIPT 81
s
solution
82
she
Solution heat exchanger, State at the outlet of the absorption pump
83
w
water, external fluid of the absorption chiller
84
x
Components of the absorption chiller: a, c, e, g
RI PT
85 1. Introduction
87
The use of absorption chillers to produce cold by means of solar thermal energy has
88
generated a high interest in the last decades; e. g. Zhai et al. [1] and Boophathi Raja and
89
Shanmugam [2] among others, where the importance of the three temperatures of
90
interchange of the absorption chiller is highlighted. The solar collectors produce hot
91
water that drives the chiller. The synchronicity between heat production and cold
92
demand makes this technology very attractive. The solar irradiance has a non-steady
93
behaviour during the day what makes necessary to actively control the system. The
94
solar thermal collectors exhibit a continuously decaying efficiency for collecting heat
95
with an increase of the temperature of the flowing water inside them. On the other hand
96
the conversion efficiency of the collected heat into cold by the absorption machine
97
(COP) typically exhibits a continuously increasing value when the hot water
98
temperature increases within the reasonable operating range, e. g. Fernández-Seara and
99
Vázquez [3]. A further increase eventually leads to a slight decrease in COP that
100
obviously is not of interest in this case; moreover some authors do not report this
101
decrease, e. g. Sun [4]. Thus, a water temperature exists that results in maximum
102
conversion of solar energy into cooling energy, quantified by SCOP, Eq. (14). Such
103
optimum value depends on operating and environmental variables, and varies
104
throughout the day. A suitable optimum driving temperature has been explored in the
105
past with different aims and different methodologies. Albers [5] performs a theoretical
AC C
EP
TE D
M AN U
SC
86
4
ACCEPTED MANUSCRIPT and experimental study where both the driving and recooling (absorber and condenser)
107
temperatures are controlled with the aim of minimizing the total cost of solar cooling.
108
This cost is the addition of fixed plus variable cost, including backup heat from a
109
district heating network and recooling fan electric consumption. Minimization was
110
performed with a specified cooling water temperature and cooling capacity (load). The
111
optimization algorithm is based on a modified characteristic temperature difference
112
method ∆∆t as the design variable, which will be explained in Section 2. It was
113
enhanced by considering internal variable losses of the real absorption machine to better
114
follow its performances, instead of constant values as in the original method. This
115
modification requires additional internal data from the machine, what is an undesirable
116
condition for commercial application. In [6] Li et al. perform a theoretical study of the
117
dependence of SCOP on the hot water temperature, evaporator temperature and
118
recooling temperature, for constant hot water flow rate and a simplified CPC collector
119
efficiency equation. A numerically solved thermodynamic absorption cycle represents a
120
generic double effect machine. From this study the optimum monthly average hot water
121
temperature is deduced for a single specific subtropical location. More straightforward
122
criteria for optimization seem desirable, especially for on-line control.
123
The optimum driving temperature has been already analytically made explicit and
124
applied to commercial H2O/LiBr absorption chillers, Lecuona et al. [7] using the
125
concept of an empirical characteristic temperature difference ∆∆t [8], Kühn and Ziegler,
126
defined in Eq. (1). The experimentally obtained ∆∆t serves to describe the cooling
127
power of the absorption chiller [8], and it is able to describe different commercial
128
absorption chillers, in both the configuration of single and double effect, as it has been
129
demonstrated by Puig-Arnavat et al. in [9], with advantages over other approximate
AC C
EP
TE D
M AN U
SC
RI PT
106
5
ACCEPTED MANUSCRIPT methods. This model has been extended to absorption chillers with adiabatic absorbers
131
[10] by Gutiérrez-Urueta et al. underlining the usefulness of the concept.
132
The most common working pair used in absorption chillers for air-conditioning is
133
H2O/LiBr. This working pair yields a good performance for air-conditioning
134
temperatures but it risks of crystallizing and it cannot produce cold under 0 ºC
135
temperatures. For temperatures under 0 ºC the common working fluid is NH3/H2O.
136
There is an alternative working fluid, NH3/LiNO3. This pair does not need a
137
rectification tower, reaches a higher efficiency in single effect cycles, e. g. Sun [11], and
138
does not suffer from crystallization risk, so that a dry cooling tower is possible. In
139
addition, the absence of water with this working fluid offers a low risk of corrosion.
140
NH3 is a natural refrigerant and LiNO3 is an inorganic salt; neither of them does
141
represent an environmental hazard when recycled at the end of their long operating life.
142
Some experimental works show the good performance of this working solution [12-15].
143
In [12] Antonopoulus and Rogdakis show that LiNO3 is superior to other salts with
144
NH3. In [13] Llamas-Guillén et al. show the feasibility for high recooling temperatures.
145
New absorbing technologies for this working pair have been explored in [14] and [15]
146
by Zacarías et al. for coping with the high viscosity of this fluid at low temperatures.
147
They take advantage of the high pressure differential.
148
In order to produce cold when the solar irradiance is not enough to satisfy the cold
149
demand it is necessary to use additional chillers, generally consuming electricity. This
150
independent backup system increases cost and complexity, difficulting the solar cooling
151
implementation. Burning a fossil fuel for helping the absorption chiller drive means net
152
direct and indirect CO2 emissions that can be higher than using mechanical compression
153
cooling, at least for single-effect absorption cycles, Fig 1 a. For a more widespread
AC C
EP
TE D
M AN U
SC
RI PT
130
6
ACCEPTED MANUSCRIPT implementation of solar cooling it seems that an integrated approach is needed. To this
155
end the hybridization of an absorption cycle with a mechanical compression cycle has
156
been attempted, using a parallel configuration of a mechanical and a thermochemical
157
compressor, e. g. Morawetz [16], but with non-known practical implementations up to
158
now. The idea is simple, when the refrigerant production by the solar driven absorption
159
cycle is not enough, extra cooling capacity can be produced in parallel by the
160
electrically driven mechanical compressor, sharing the condenser and evaporator.
161
Interactions between both cycles have not been much studied. The very large specific
162
volume of H2O vapour at the usual working temperatures precludes basing the hybrid
163
cycle on the H2O/LiBr working pair. On the other hand, the working pair NH3/LiNO3
164
offers the possibility of hybridization as there is much experience on the suitable NH3
165
compressors; the pressure levels are acceptable and oil-less compressors and pumps are
166
available.
167
Ventas et al. [17] showed another possibility of hybridization by pressure boosting a
168
single effect absorption cycle, Fig 1 b. In this configuration the compressor is installed
169
between the evaporator and the absorber keeping the same evaporation temperature (and
170
pressure) but forcing a higher absorption pressure, in favour of the absorption process.
171
The resulting electrical COP (COPe) is high, e. g. [17]. Considering the same upper part
172
of the cycle, the result is a wider concentration change in the absorber and consequently
173
a higher cooling capacity for the same external temperatures. Modulating the booster
174
compressor pressure ratio pr gives control of the refrigerant mass flow, thus allowing a
175
control of the cooling capacity. From another perspective, the NH3/LiNO3 pair has been
176
studied for this configuration allowing to reduce the driving temperature up of 24 ºC for
177
pr = 2.0, maintaining the same COP and cooling capacity as the regular single effect
AC C
EP
TE D
M AN U
SC
RI PT
154
7
ACCEPTED MANUSCRIPT cycle [17]. That reduction in temperature seems to be interesting for improving the
179
overall efficiency of a solar cooling facility. If a reduction in driving temperature is not
180
the scope of boosting, an increase in cooling capacity is observed for the same external
181
temperatures. Thus, pressure boosting offers an additional controllable degree of
182
freedom for absorption machines for increasing capacity without wasting solar heat.
183
Another cycle that has been studied with NH3/LiNO3 allowing increasing the pressure
184
of the absorber is the use of an ejector within the cycle; only as a booster [18] or as a
185
simultaneous adiabatic absorber [19], both by Vereda et al.
186
Within this framework, the aim of this work is to obtain and to discuss how the
187
optimum hot water temperature evolves during reference sunny days, in this case for
188
Madrid, central Spain, using the most common technology available: the combination of
189
high efficiency flat plate collectors and single effect machines. From these results the
190
possible strategies of temperature control for obtaining the maximum cold production
191
are studied. Three types of absorption chillers are studied and the results are compared
192
in order to know their behaviour for a common air-conditioning purpose: 1) H2O/LiBr
193
single effect absorption chiller; 2) NH3/LiNO3 single effect absorption chiller; and 3)
194
NH3/LiNO3 single effect absorption chiller hybridized with a low pressure compressor
195
booster [17]. To allow the same basis for comparison, the data needed are obtained in
196
all cases from a detailed thermodynamic cycle and their behaviour is synthesized by
197
means of the modified characteristic temperature difference ∆∆t so that a
198
straightforward calculation and optimization is allowed, even for the hybrid cycle. The
199
outcome of this first study is of use to establish strategies for controlling the absorption
200
machines in a solar cooling arrangement and gives the maximum production profile
201
along the day. Also it will indicate whether the emerging NH3/LiNO3 working pair is
AC C
EP
TE D
M AN U
SC
RI PT
178
8
ACCEPTED MANUSCRIPT competitive against the more usual H2O/LiBr for air conditioning, either in terms of
203
efficiency and operating temperature for the solar collectors. Moreover, this paper
204
quantifies the gain obtained by hybridizing this cycle with a low pressure compressor
205
booster.
206
2. ∆∆t model for the absorption chillers
207
RI PT
202
2.1. ∆∆t of 1) H2O/LiBr and 2) NH3/LiNO3 conventional single effect absorption chiller
209
The cooling capacity of an absorption machine can be formulated as a linear
210
dependence on the characteristic temperature difference ∆∆t within the normal
211
operating range. The characteristic temperature difference depends on the inlet to outlet
212
averaged external temperatures of the absorption chiller heat exchangers. The ones
213
corresponding to condenser and absorber are the same tac (thus in parallel balanced
214
cooling circuits), being calculated as the averaged temperature of condenser and
215
absorber tac =
216
for the generator is tg. From its inception in Helman et al. [20] it is a linear function
217
using two empirical constants, a and b:
M AN U
TE D
EP
tc + t a , from now called for simplicity tc = tac. For the evaporator is te and 2
AC C
218
SC
208
∆∆t = t g − a tc + b te
(1)
219
These constants have been obtained fitting the experimental data resulting from a steady
220
state operating single-effect absorption chiller (Fig. 1 a) of the H2O/LiBr type [8],
221
corresponding the constant values = 2.5 and = 1.8.
222
A thermodynamic model for H2O/LiBr has been carried out to determine whether the
223
driving power and cooling power (capacity) can be described with a linear
9
ACCEPTED MANUSCRIPT dependence on ∆∆t. From a thermodynamic cycle model ∆∆t has been obtained in [9]
225
and compared to experimental results from commercial machines. The results showed
226
that the characteristic temperature, with = 2.3031 and = 1.3034 , allowed
227
describing with reasonable accuracy the performance of the commercial absorption
228
chillers tested. This means that the values of those coefficients are no longer the original
229
values proposed but, according to the modified method based on ∆∆t, [8] and [9] among
230
others, this meaning that ∆∆t can be < 0.
231
The thermodynamic model is based on energy balances and heat transfer quasi-steady
232
equations, constant overall UA and logarithmic temperature difference ∆Tlm, in every
233
counter-current heat exchanger of the absorption chiller: absorber, generator, solution
234
heat exchanger, evaporator and condenser, thus involving the external temperatures.
235
These equations are summarized as follows, denoting i and o respectively inlet and
236
outlet:
237
Internal side:
SC
M AN U
TE D
= , ℎ − ℎ
241
242
AC C
240
External side:
(2)
EP
238 239
RI PT
224
= , ℎ − ℎ
(3)
Q& x = UAx ∆Tmlx
(4)
Heat transfer equation:
243
x corresponds to every component, x = e (evaporator), x = c (condenser), x = a
244
(absorber), x = g (generator), x = she (solution heat exchanger). h is the specific
10
ACCEPTED MANUSCRIPT enthalpy of the internal or external fluids, either solution or refrigerant. Variables are
246
marked with the subscript s for internal flow. For external water flow, they are marked
247
with the subscript w.
248
The model has been described in detail in [17], but in this paper there is a small
249
modification; saturation state at the outlet of the evaporator, condenser, generator and
250
absorber has been imposed. The equation set is solved with the software EES® [21]. It
251
incorporates the input values that have been selected from the simulation of a single-
252
effect absorption chiller of NH3/LiNO3 [17]. Table 1 summarizes those values.
253
For obtaining the performance of the selected absorption chiller, the external inlet
254
temperatures of the four plate heat exchangers have been varied. The absorber and
255
condenser inlet temperatures, have been taken as ta,i = tc,i = 30 - 35 ºC, the evaporator
256
inlet temperature te,i = 5 - 10 - 15 ºC and the generator inlet temperature from the
257
specific activation temperature up to 30 ºC above that value, being the overall range of
258
tg,i from 48 to 100 ºC. This absorption chiller has a capacity of 7.08 kW for tg,i = 84 ºC,
259
te,i = 10 ºC and and tc,i = 30 ºC. The software EES® [21] gives the properties of
260
H2O/LiBr, using the formulation of the work [22] by Patek and Klomfar. This model
261
has been experimentally verified in Ventas et al. [23].
262
The values of the constants in the characteristic temperature difference have been
263
obtained by means of a multivariable linear regression to the results of the
264
thermodynamic cycle [23], resulting in:
265
AC C
EP
TE D
M AN U
SC
RI PT
245
∆∆tH2O/ LiBr = tg − 2.322 tc + 1.342 te
(5)
11
ACCEPTED MANUSCRIPT The constant values a and b obtained with the model are quite similar to those obtained
267
in [9], although, the values are different from the results given in [8], as already
268
commented. An absorption chiller working with solar heat should operate at relatively
269
low ∆∆t values [7] to avoid excessive collectors’ temperature. For this reason the
270
cooling power and driving powers have been correlated with the thermodynamic model
271
results with ∆∆ < 10 ºC. The output of this correlation is shown below, as
272
characteristic equations: 0.310 kW Q& e = ⋅ ∆∆t H 2O / LiBr + 1.530 kW ºC
274
0.326 kW Q& g = ⋅ ∆∆t H 2O / LiBr + 1.956 kW ºC
M AN U
273
SC
RI PT
266
(6)
(7)
These equations show an asymptotically increasing COP with tg, what is only valid for
276
the range of interest for solar cooling, as explained in the Introduction section. The
277
cooling power is described with a linear dependence on ∆∆t with a smaller variance
278
than the driving power, as also observed in [8] and [9].
279
Now the model of the same single-effect cycle is applied to the NH3/LiNO3 solution as
280
working fluid, keeping constant the input variables shown in Table 1, except that the
281
solution mass flow rate now is = 0.058 kg s-1, according to the lower latent heat of
282
ammonia. The condenser and absorber inlet temperatures have been taken as ta,i = tc,i =
283
25 - 30 - 35 ºC. The evaporator inlet temperature taken are te,i = 5 - 10 - 15 ºC and the
284
generator inlet temperature from the activation temperature to 60 ºC more than that
285
value, being the range of tg,i from 42 to 122 ºC. This absorption chiller has a capacity of
286
6.08 kW for tg,i = 84 ºC, te,i = 10 ºC and tc,i = 30 ºC. The solution properties used for the
287
model are those given by Infante Ferreira [24].
AC C
EP
TE D
275
12
ACCEPTED MANUSCRIPT
290
∆∆t NH3 / LiNO3 = t g − 2.225 tc + 1.198 te The cooling power and the driving power as a function of ∆∆ are shown below:
291
0.3 kW Q& e = ⋅ ∆∆t NH 3 / LiNO3 + 1.695 kW ºC
292
0.383 kW Q& g = ⋅ ∆∆t NH 3 / LiNO3 + 2.732 kW ºC
(9)
(10)
2.2. ∆∆t of 3) NH3/LiNO3 single effect hybridized with a low pressure
M AN U
293
(8)
RI PT
289
The characteristic temperature difference obtained for NH3/LiNO3 as working fluid is:
SC
288
booster compressor
295
In this section a new characteristic equation is determined for the hybrid cycle. The
296
difference between the hybrid cycle and the single effect conventional absorption chiller
297
is the use of a mechanical compressor between the evaporator and the absorber. This
298
cycle is in detail described and analysed in [17], Fig. 1 b.
299
The low pr mechanical compressor helps the thermochemical compressor reaching the
300
pressure increase needed by the solution. The thermochemical compressor is working as
301
if it being a part of a single-effect absorption chiller but as having a higher evaporation
302
pressure Pe and, correspondingly, as it would work at a higher evaporation temperature.
303
This temperature would be the saturation temperature at the outlet pressure of the
304
mechanical compressor T’e instead of the real evaporation temperature Te. For
305
calculating how the equivalent saturation temperature changes with pressure, the
306
ammonia properties from the EES® software [21] have been used. The correlation
AC C
EP
TE D
294
13
ACCEPTED MANUSCRIPT 307
obtained is for external evaporation temperatures from 5 to 10 ºC and pr = 1-1.2-1.4-
308
1.6-1.8-2:
T 'e = pr 0.1054 Te
;
pr =
Pa Pe
(10)
RI PT
309
The evaporation absolute temperature of the evaporator Te [K] is an internal temperature
311
of the cycle but it is considered that a virtual external evaporator average temperature
312
follows the behaviour of the internal temperature. For this reason the external average
313
temperature of the evaporator for the characteristic equation t’e [ºC] is defined by means
314
of Eq. (2) using te:
M AN U
SC
310
t 'e = (te + 273.16 ºC) pr 0.1054 − 273.16 ºC
315
(11)
Thus, the equivalent characteristic temperature for the hybrid cycle can now be written
317
in a new way, on the grounds of the method for single effect cycles [7] to [9] as:
TE D
316
∆∆thybrid = t g − a tc + b t 'e
318
(12)
The values of the constants a and b selected are the same than those found for a single-
320
effect absorption chiller, Eq. (8).
321
The same input variables, Table 1, than the single-effect cycle with NH3/LiNO3 have
322
been used, but adding a compressor with an isentropic efficiency η = 0.7. The vapour
323
overheating because of the internal irreversibilities is considered on the thermodynamic
324
cycle.
325
It was checked that the same correlations for and for ∆∆ < 5 ºC, indicated in
326
Eqs. (9) and (10), can be used for the hybrid cycle, but using ∆∆thybrid,.
AC C
EP
319
14
ACCEPTED MANUSCRIPT Eq. (11) indicates that increasing pr increases ∆∆thybrid, thus increasing the cooling
328
capacity through Eq. (10). At the same time increases, according to Eq. (11). The
329
electric power of the booster compressor is given by the thermodynamic cycle and is
330
defined by the ratio of cooling power versus work power consumption of the
331
compressor Q& e / W&c that depends only on the pressure ratio, as demonstrated in [17].
332
The electrical COP of the booster compressor, COPe =∆Q&e / W&c , meaning this the
333
increase of capacity over the conventional non-boosted cycle, as defined in [17], is high
334
for low values of ∆∆t. For low
335
in [17] it is demonstrated that this ratio is constant for all the temperatures involved.
336
Actually, the lower is pr, the higher %&' is.
337
3. Solar cooling model
338
In [7] the conditions for maximizing the instantaneous cooling power for a prescribed
339
solar irradiance on the collectors, using a linear characteristic curve for the solar
340
collector efficiency and a ∆∆t model have been analytically obtained. No thermal inertia
341
is considered. This means maximizing the solar coefficient of performance SCOP:
SC
where the single effect cycle is not producing cold,
EP
TE D
M AN U
, ,
SCOP = Q&e / ( GT As )
(14)
AC C
342
RI PT
327
343
SCOP is the product of the solar collector energy efficiency times the COP of the
344
absorption machine and times the hydronic facility energy efficiency, owing to heat
345
losses and the associated temperature drops in the thermal fluid. This model is of only
346
relative accuracy but offers a tool for discriminating general trends and offering guides
347
for further study.
15
ACCEPTED MANUSCRIPT The model for the solar collectors and hydronic circuits uses the same values than in
349
[7], corresponding to high efficiency flat plate collectors of contemporary technology.
350
The application of this model to two real absorption machines versus time is offered in
351
[7].
352
In this paper, sunny days have been considered as representative of the maximum
353
possible. Madrid (Spain) has been selected as a continental Mediterranean climate with
354
dry summers. It is located at 687 m altitude. Day 196 (mid-July) has been selected as
355
representative of the cooling season with an average maximum tatm = 31.2 ºC and
356
minimum of 18.9 ºC, as can be seen in Figs. 2 and 3. A second day two month later
357
(mid-September), with lower temperatures and solar irradiance, serves as an end-of-
358
season example. A Hottel correlation for solar irradiance along the day has been used,
359
[25] and elsewhere. This yields GT = 1,082.0 W m-2 of maximum total irradiance on the
360
optimally tilted fixed position collector for the selected mid-July day at noon.
361
4. Results and discussion
362
Figs. 2 and 3 show: the optimum driving temperature tg,op versus solar time from sunrise
363
to sunset, the atmospheric temperature tatm and the minimum temperature for cold
364
production, namely the activation temperature tg,0. Fig. 2 shows the results for the mid-
365
July day for the three cycles, 1) single-effect H2O/LiBr, 2) single-effect NH3/LiNO3 and
366
3) NH3/LiNO3 single effect hybridized with a low pressure compressor booster with pr
367
= 1.5. Fig. 3 depicts the same results but for the mid-September day. These figures show
368
that the optimum temperature smoothly grows above the activation temperature from an
369
instant about an hour after sunrise toward the early afternoon, decreasing afterwards
370
toward about an hour before sunset when the machine stops once tg,op = tg,0. The results
371
for the H2O/LiBr cycle show slightly higher tg,op than the NH3/LiNO3 cycle, being both
AC C
EP
TE D
M AN U
SC
RI PT
348
16
ACCEPTED MANUSCRIPT in the range of 49 – 86 ºC for mid-July and 41-76 for mid-September; these lower
373
values occur mainly because of the lower ambient temperature. The NH3/LiNO3 single
374
effect chiller hybridized with a low pressure compressor booster with pr = 1.5, shows
375
tg,op about 16 ºC lower than for the other cycles, what implies a less thermally stressed
376
solar facility, being this temperature in the range of 33 to 72 ºC for mid-July and 25-62
377
for mid-September.
378
Fig. 4 shows the resulting time-varying optimal SCOP, and also with time-constant tg of
379
70 ºC, 80 ºC and 90 ºC along the whole sunshine hours for the single-effect NH3/LiNO3
380
cycle, producing cold only when they are higher than tg,0. There is some loss in SCOP
381
along time when they are different to tg,op, demonstrating the advantage of operating at
382
the instantaneous tg,op. This loss is more evident for tg < tg,op than for tg > tg,op owing to
383
the steep decrease of COP for lower hot water temperatures [7]. The figure also shows
384
that either pumping half the nominal mass flow rate through the solar collectors at tg,op,
385
a possible loss in SCOP is the result. For the case of pumping the double of the nominal
386
mass flow rate there are hardly any losses and for this reason it is not shown in the
387
figure. This paper does not include the possibility of operating at variable mass flow
388
rate neither at variable evaporation temperature te as part of a multi-variable
389
optimization. But they can change along time in a prescribed way and the methodology
390
is still valid if the corresponding parameters are available.
391
Fig. 5 shows the resulting SCOP along solar time for the three cycles operating at tg,op,
392
exhibiting maximum values around 0.4 – 0.5. All the cycles show a similar time
393
evolution of the instantaneous maximum SCOP in spite of the higher COP curve of the
394
H2O/LiBr machine. This is a consequence of the combination of a) a lower ∆∆t for
395
activation, namely ∆∆t0, of the NH3/LiNO3 cycle, -5.65 ºC in front of -4.94 ºC for
AC C
EP
TE D
M AN U
SC
RI PT
372
17
ACCEPTED MANUSCRIPT H2O/LiBr, giving a plus for the former, and b) a slightly lower sensitivity of COP to
397
∆∆t of the NH3/LiNO3 cycle, giving a minus, as Eqs. (6) and (9) show.
398
For the H2O/LiBr machine modelled in this work, Eq. (6), the solar field dimensions
399
would be 9.95 m2 to produce 5.45 kW at midday. This result has been obtained with the
400
optimum ∆∆t and the SCOP shown in Fig. 5. For the NH3/LiNO3 single effect machine
401
shown in Eq. (9) the solar field dimensions would be 10.54 m2 to produce 4.72 kW at
402
midday. Other values can be embraced by just escalation.
403
The resulting SCOP for the H2O/LiBr single-effect machine is higher than for the
404
NH3/LiNO3 single-effect machine. This is attributed to a higher raising COP curve for
405
the H2O/LiBr machine when tg increases, Eqs. (6) and (7). On the other hand the hybrid
406
cycle starts to produce cold sooner and stops later than the other two cycles. The
407
maximum SCOP is lower for the hybrid cycle than for the H2O/LiBr single effect cycle,
408
but the same than the NH3/LiNO3 single effect cycle. The main difference is that the
409
hybrid cycle maintains a flatter behaviour of SCOP near the maximum. The averaged
410
SCOP from 6:00 h and 18:00 h solar time of every cycle, obtained from Fig. 5, is 0.411
411
for the H2O/LiBr single effect cycle, 0.336 for the NH3/LiNO3 single effect cycle and
412
0.381 for the hybrid cycle with pr = 1.5.
413
Figure 6 show the day accumulated cold production per collector one meter surface
414
[J/m2] versus an imposed time-constant driving temperature
415
day. This figure shows the results for the three cycles shown before: single-effect
416
H2O/LiBr, single-effect NH3/LiNO3, and NH3/LiNO3 hybrid cycle with pr = 1.5. This figure
417
incorporates a new curve showing the results of the hybrid cycle with pr = 2.0. The first key
418
result is that the SCOP curve around maximum is quite smooth, indicating that the
419
inaccuracies of the model parameters or in the control system are not crucial. One can
AC C
EP
TE D
M AN U
SC
RI PT
396
,
also for the mid-July
18
ACCEPTED MANUSCRIPT observe that too high tg stems into an almost linear SCOP decay caused by an almost
421
constant COP and linearly decreasing collector efficiency. On the other hand, a too low
422
tg derives into a fast decreasing SCOP.
423
The figure also show that there is an optimum time-constant temperature maximizing
424
the cold production, depending on the solar and ambient conditions. This is evident
425
when comparing with the curve for the mid-September day, Fig. 7. Moreover, operating
426
at a too high constant tg there is less risk to obtain a lower cold production than
427
operating at a too low constant tg. This seems to explain the current practice of operating
428
at somehow elevated hot water temperatures.
429
Figs. 6 and 7 also show that operating with the time-variable tg,op a higher production is
430
obtained. But the gain is modest within our constraints. This suggests that operating at a
431
specific constant driving temperature is an option, simplifying the control system, but
432
this temperature must of the appropriate value for the climate, the solar irradiance and
433
te. Another more elaborate option could be approaching the curve of tg,op with morning
434
and evening smooth ramps and setting a constant value for the middle of the assumed
435
sunny day. The ∆∆t model yields the clues on how to operate with a combination of the
436
influencing temperatures.
437
Comparing the three cycles a conclusion can be drawn. The NH3/LiNO3 cycle produces
438
at tg,op 10.5 MJ m-2 of cold for the mid-July day and 9.2 MJ m-2 for the mid-September
439
day. Meanwhile the H2O/LiBr cycle produces 12.8 MJ m-2 for the mid-July day and
440
11.2 MJ m-2 for the mid-September day, 22 % and 23 % more than the NH3/LiNO3
441
cycle respectively. Hybridizing the NH3/LiNO3 cycle with a booster compressor this
442
loss can be reduced or even overcome, not deteriorating the efficiency of the absorption
443
cycle [11]. This hybrid cycle totalizes a cold production for the mid-July day of 11.9 MJ
AC C
EP
TE D
M AN U
SC
RI PT
420
19
ACCEPTED MANUSCRIPT m-2 for pr = 1.5 and 12.9 MJ m-2 for pr = 2.0, for the same day, this is respectively 8 %
445
lower and 0.6 % higher than using the single-effect H2O/LiBr cycle; for this reason only
446
one line is represented in Fig. 6 for the hybrid cycle with pr = 2 and single-effect
447
H2O/LiBr cycle. This improvement has been achieved thanks to the electricity
448
consumption of the compressor. It is necessary to evaluate the quantity of energy
449
consumed for that in a day. For the case of pr = 1.5 the ratio of cooling power versus
450
power consumption results to be constant, being in this case Q& e / W&c = 14.5 and being
451
of identical value of COPe = 14.5, so that the hybrid cycle was working at tg lower than
452
the activation temperature of the conventional single-effect absorption cycle [17]. The
453
Q& e / W&c result has been obtained by means of the thermodynamic model. The work
454
consumption is 0.819 MJ m-2 in July and 0.721 MJ m-2 in September. For the case of pr
455
= 2.0, Q& e / W&c is also kept constant, being in this case Q& e / W&c = 8.07 and, as well as for
456
pr = 1.5. This ratio sensibly coincides with the electrical coefficient of performance
457
COPe = 8.07, being the work consumption of the compressor 1.45 MJ/m-2 in July and
458
1.29 MJ/m-2 in September. The resulting high COPe guarantees CO2 reductions over a
459
system solely based on mechanical compression cooling consuming electricity from the
460
grid.
461
The hybrid cycle curves show a shift towards even lower constant tg for which the cold
462
production losses are minimum with respect the optimum driving temperature. This is
463
the result of the higher pr, so that the maximum production appears at tg = 58 ºC for
464
July and 47 ºC for September for pr = 2.0. For the conventional single effect cycles this
465
signifies 25 ºC lower with H2O/LiBr and 24 ºC lower with NH3/LiNO3.
AC C
EP
TE D
M AN U
SC
RI PT
444
20
ACCEPTED MANUSCRIPT Running the model for other days, the results indicate that when the date separates from
467
about the summer solstice the optimum constant temperature tg decreases. They also
468
indicate a stronger convenience to increase pr to increase the capacity over solar alone.
469
This reveals that the hybrid cycle incorporates solar heat in an effective way combining
470
it with work to fulfil the user needs. For the conventional non-boosted cycle it could be
471
less and less possible to profit from solar cold. This singular advantage of boosting
472
using the hybrid cycle is a consequence of higher collector efficiencies caused by the
473
lower tg.
474
The thermodynamic model used in Section 2 for each cycle is now used to show the
475
cooling power obtained instantaneously for the optimum temperature determined. The
476
results are compared to the cooling power given for the approximate ∆∆t model along
477
the mid-July day in order to explore the accuracy of the ∆∆t model. Fig. 8 a shows the
478
results of e for the mid-July day with respect the solar angle, for H2O/LiBr, and for
479
both cases: the thermodynamic model and the ∆∆t model. The total energy obtained
480
along the day is 3.6 % lower for the case of the thermodynamic model than the ∆∆t
481
model. For the NH3/LiNO3 single effect cycle the total energy obtained is
482
underestimated a 5.8 % by the ∆∆t model compared to the thermodynamic model. On
483
the other hand, for the NH3/LiNO3 single effect cycle hybridized with a low pressure
484
compressor booster with pr = 1.5 the ∆∆t model underestimates a 7.6 % of the total
485
energy obtained, Fig. 8 b. For the case of the NH3/LiNO3 single effect absorption cycle
486
hybridized with low pressure compressor booster with pr = 2.0 the ∆∆t model
487
underestimates by 14.9 % the total energy. It can be said that the accuracy of the ∆∆t
488
model is quite high for the single effect cycles but its accuracy decreases for the hybrid
489
cycle when the pressure ratio of the hybrid cycle increases.
AC C
EP
TE D
M AN U
SC
RI PT
466
21
ACCEPTED MANUSCRIPT Correcting the ∆∆t model results with the thermodynamic model for the July cases
491
shown in Fig. 6, the total energy obtained would be 11.07 MJ m-2 for the NH3/LiNO3
492
single-effect cycle, 12.35 MJ m-2 for the H2O/LiBr single-effect cycle, 12.76 MJ m-2 for
493
the hybrid with pr = 1.5 cycle and 14.81 MJ m-2for the hybrid with pr = 2.0 cycle. With
494
the corrected results the hybridization cycle for pr = 2.0 produces a 15.6 % more cold
495
than the single-effect H2O/LiBr cycle. In order to obtain this improvement a work
496
consumption is needed, being 1.67 MJ m-2 for the pr = 2.0 case in July.
497
5. Conclusions
498
This paper offers the results of modelling the instantaneous solar cold production during
499
two sunny summer days using: 1) a H2O/LiBr single effect cycle, 2) a NH3/LiNO3
500
single effect cycle, and 3) a NH3/LiNO3 single effect cycle hybridized with a low
501
pressure compressor booster. The resulting cooling capacity and driving heat power are
502
fitted with a simple empirical model based on the modified ∆∆t concept instead of the
503
thermodynamic cycle, signifying an extension of the concept for hybrid booster cycles.
504
This allows an analytical maximization of cold production. The low side is that some
505
accuracy is lost, but fortunately the optimized variables show a smooth hill around
506
maximum, so that the error seems acceptable in front of the optimization capability
507
obtained. The reasons for the accuracy loss when pr increases have not been
508
investigated in detail, but one reason could be the vapor temperature increase through
509
the compressor as a result of its irreversibility; this loss was not considered in the
510
original ∆∆t method.
511
The results indicate that:
AC C
EP
TE D
M AN U
SC
RI PT
490
22
ACCEPTED MANUSCRIPT 512
•
Maximum solar cold production requires a time varying temperature tg,op for driving the absorption machine that requires finely controlling the working of
514
the system. During a sunny day it grows towards an instant some hours after
515
noon. The resulting COP and SCOP evolves in the same manner. The
516
instantaneous cold capacity shows a more peaky behaviour. Primary circuit flow
517
rate variation seems customary for reaching tg,op. •
Using a fixed tg, implies a loss in the daily production that is not substantial if
SC
518
RI PT
513
the temperature is chosen as suitable for the day. This simplifies the chiller
520
control and partially reduces the thermal inertia effects. The optimum fixed
521
temperature has to be determined at the beginning of the day depending on the
522
meteorological forecast. It could be corrected along the day using on-line
523
meteorological information. •
Cooling power under optimum solar driving temperature is significantly lower
TE D
524
M AN U
519
than the usual nominal power of absorption chillers, which corresponds to
526
higher values of ∆∆t than the one corresponding to tg,op. This seems relevant for
527
dimensioning.
529 530 531
•
Solar cooling using the NH3/LiNO3 working pair inside a hybrid booster cycle is
AC C
528
EP
525
feasible, promising and convenient, as it operates efficiently with low cost flat plate collectors. This setup is capable of covering a wide range of cooling demands, even in the case of no solar irradiance. Its produces 15.6 % more cold
532
than the single-effect H2O/LiBr cycle for air conditioning, using a moderate
533
pressure ratio of 2.0.
23
ACCEPTED MANUSCRIPT 534
As a main conclusion solar cooling using the NH3/LiNO3 working pair is feasible and
535
attractive using just the simplest solar setup.
536
Acknowledgements
538
The financial support of this study by the Spanish Ministry of Education and Science
539
research grant ENE2009-11097 is greatly appreciated.
540
RI PT
537
References
542
[1] Zhai X.Q., Qu M., Li Y., Wang R.Z. A review for research and new design options
543
of solar absorption cooling systems. Renew and Sustainable Energy Rev 15 (2011)
544
4416–4423.
M AN U
SC
541
[2] Boopathi Raja V., Shanmugam V. A review and new approach to minimize the
546
cost of solar assisted absorption cooling system. Renew and Sustainable Energy
547
Rev 16 (2012) 6725–6731.
TE D
545
[3] Fernández-Seara J. A., Vázquez M.. Study and control of the optimal generation
549
temperature in NH3/H2O absorption refrigeration systems. Appl Therm Eng, 21
550
(2001) 343-357.
552 553 554 555
[4] Sun, D. Comparison of the performances of NH3-H20, NH3-LiNO3 and NH3-
AC C
551
EP
548
NaSCN absorption refrigeration systems. Energy Convers. Mgmt (1998), 39 (5/6), 357–368.
[5] Albers J. New absorption chiller and control strategy for the solar assisted cooling system at the German federal environment agency Int J of Refrig 39 (2014) 48-56
24
ACCEPTED MANUSCRIPT 556
[6] Li Z., Ye X., Liu J. Optimal temperature of collector for solar double effect
557
LiBr/H2O absorption cooling system in subtropical city based on a year round
558
meteorological data. Appl Therm Eng, 69 (2014) 19-28.
560
[7] Lecuona, A., Ventas, R., Venegas, M, Zacarías, A., Salgado, R. Optimum hot water for absorption solar cooling, Sol Energy 83 (2009) 1806-1814.
RI PT
559
[8] Kühn, A., Ziegler, F. Operational results of a 10 kW absorption chiller and
562
adaptation of the characteristic equation. International Conference of Solar-Air
563
Conditioning, 70-74, 6-7 October 2005, Kloster Banz, Germany.
SC
561
[9] Puig-Arnavat, M., López-Villada, J., Bruno, J.C., Coronas, A. Analysis and
565
parameter identification for characteristic equation of single- and double-effect
566
absorption chillers by means of multivariable regression. Int J of Refrig 33 (2010)
567
70-78.
M AN U
564
[10] Gutierrez-Urueta, Rodríguez, P., Ziegler, F., Lecuona, A., Rodriguez-Hidalgo,
569
M.C. Extension of the characteristic equation to absorption chillers with adiabatic
570
absorbers. Int J of Refrig, 35 (2012) 709-718.
TE D
568
[11] D. W. Sun. Comparison of the performance of NH3-H2O, NH3-LiNO3 and NH3-
572
NaSCN absorption refrigeration systems. Energy Convers Manag 39 (5/6) (1998)
573
357-368.
EP
571
[12] Antonopoulos, K. A., Rogdakis, D. E. Performance of solar driven ammonia-
575
lithium nitrate and ammonia-sodium thiocyanate absorption systems operating as
576
AC C
574
coolers or heat pumps in Athens. Appl Therm Eng, 16 (1996) 127-147.
577
[13] Llamas Guillén, S.U., Cuevas, R., Best, R., Gómez, V. H. Experimental results of
578
direct air-cooled ammonia-lithium nitrate absorption refrigeration system, Appl
579
Therm Eng 64 (2014) 362-369.
25
ACCEPTED MANUSCRIPT 580
[14] Zacarías, A., Venegas, M., Ventas, R., Lecuona, A. Experimental assessment of
581
ammonia adiabatic absorption into ammonia-lithium nitrate solution using a flat
582
fan nozzle, Appl Therm Eng. 31 (2011) 781-790.
583
[15] Zacarías, A.,Venegas, M., Lecuona, A., Ventas, R. Experimental evaluation of ammonia adiabatic absorption into ammonia-lithium nitrate solution using a fog
585
jet nozzle, Appl Therm Eng 50 (2013) 3569-3579.
586 587
RI PT
584
[16] Morawetz, M., 1989. Sorption-compression heat pumps. Int J of Energy Res, 13 (1989) 83-102.
[17] Ventas, A., Lecuona, A., R., Zacarías, Venegas, M,. Ammonia-lithium nitrate
589
absorption chiller with an integrated low-pressure compression booster cycle for
590
low driving temperatures. Appl Therm Eng 30 (2010) 1351-1359.
M AN U
SC
588
591
[18] Vereda, C., Ventas, R., Lecuona, A., Venegas, M. Study of an ejector-absorption
592
refrigeration cycle with an adaptable ejector nozzle for different working
593
conditions, Appl Energy 97 (2012) 305-312.
[19] Vereda, C, Ventas, R., Lecuona, A., Lopez, R. Single-effect absorption cycle
595
boosted with an ejector-adiabatic absorber using a single solution pump 38 (2014)
596
22-29.
TE D
594
[20] Helman, H.M., Schweigler, C., Ziegler, F. A simple method for modelling the
598
operating characteristics of absorption chillers. Seminar Eurotherm nº 59,
599
Thermodynamics, heat and mass transfer of refrigeration machines and heat
601 602
AC C
600
EP
597
pumps. 6-7 July 1998, 219-226.
[21] Klein, S. A., Alvarado, F. Engineering Equation Solver, v. 8.186-3D, F-Chart Software, Middleton, WI, USA, 1999.
603
[22] Patek, J., Klomfar, J. A computationally effective formulation of the
604
thermodynamics properties of LiBr-H2O solutions from 273 to 500 K over full
605
composition range. Int J of Ref 29 (2006) 566-578.
26
ACCEPTED MANUSCRIPT 606
[23] Ventas, R., Vereda, C., Lecuona, A., Venegas, M. Experimental study of a
607
thermochemical compressor for an absorption/compression hybrid cycle. Appl
608
Energy 97 (2012) 297-304. [24] C.A. Infante Ferreira, Thermodynamic and physical property data equations for
610
ammonia-lithium nitrate and ammonia-sodium thiocyanate solutions. Sol Energy 2
611
(1984) 231-236.
613
[25] Duffie J. A., Beckmann W. A. Solar Engineering of Thermal Processes (1980), John Wiley & Sons. Hoboken, New Jersey, USA.
SC
612
RI PT
609
AC C
EP
TE D
M AN U
614
27
ACCEPTED MANUSCRIPT Table 1. Data for the thermodynamic cycle. Input Variable Value Input Variable
Value
0.35 kg s-1
UAc
3.0 kW K-1
,
0.40 kg s-1
UAe
2.5 kW K-1
,
0.17 kg s-1
UAg
1.8 kW K-1
0.028 kg s-1
UAshx
1.4 kW K-1
UAa
2.25 kW K-1
EP
TE D
M AN U
SC
RI PT
,( = ,
AC C
615 616
28
ACCEPTED MANUSCRIPT
RI PT
617
SC
618
Figure 1 Pressure versus temperature diagram of a) single effect absorption cycle b)
620
single effect absorption cycle hybridized with low pressure compressor booster.
M AN U
619
AC C
EP
TE D
621
29
ACCEPTED MANUSCRIPT 100 90 80 70 60
t (ºC) 50 40
20
tg,op SE H2O/LiBr
tg,op SE NH3/LiNO3
tg,op hybrid pr = 1.5
10
tg,0 SE H2O/LiBr
tg,0 SE NH3/LiNO3
tg,0 hybrid pr =1.5
tatm July
0 6
7
8
9
10
11
12
solar time (h)
13
14
15
16
17
18
EP
TE D
M AN U
SC
Figure 2. tg,op , tg,0 and tatm [ºC] versus solar time [h] for the mid-July day and for the three cycles: single-effect H2O/LiBr, single-effect NH3/LiNO3, and NH3/LiNO3 hybrid cycle with pr = 1.5.
AC C
622 623 624 625 626
RI PT
30
30
ACCEPTED MANUSCRIPT 90 80 70 60 50
t (ºC) 40
20 10 6
tg,op SE NH3/LiNO3
tg,op hybrid pr = 1.5
tg,0 SE H2O/ LiBr
tg,0 SE NH3/LiNO3
tg,0 hybrid pr =1.5
7
8
9
10
11
12
solar time (h)
13
14
15
16
17
18
EP
TE D
M AN U
SC
Figure 3. tg,op , tg,0 and tatm [ºC] versus solar time [h] for the mid-September day and for the three cycles: single-effect H2O/LiBr, single-effect NH3/LiNO3, and NH3/LiNO3 hybrid cycle with pr = 1.5.
AC C
627 628 629 630 631
tg,op SE H2O/LiBr tatm September
0
RI PT
30
31
ACCEPTED MANUSCRIPT 0.5
0.4
0.3
SCOP SCOP with tg,op
0.2
SCOP with tg = 70 º C
0.1
SCOP with tg = 80 ºC SCOP with tg = 90 ºC 0.0 6
7
8
9
10
11
12
solar time (h)
13
14
RI PT
SCOP with tg,op and half nominal mass flow rate
15
16
17
18
Figure 4. Solar coefficient of performance SCOP [-] versus solar time for the mid-July
634
day, single-effect NH3/LiNO3 cycle. 5 different operation possibilities: tg,op, tg,op using half
635
nominal mass flow rate of the solar collectors, constant driving temperatures of tg = 70 ºC, tg =
636
80 ºC and tg = 90 ºC.
M AN U
SC
632 633
AC C
EP
TE D
637
32
ACCEPTED MANUSCRIPT 0.6 0.5 0.4
SCOP
0.3
SCOP with tg,op SE H2O/LiBr
0.1
SCOP with tg,op SE NH3/LiNO3
SCOP with tg,op hybrid pr = 1.5 0.0 6
7
8
9
10
11
RI PT
0.2
12
solar time (h)
13
14
15
16
17
18
Figure 5. Solar coefficient of performance SCOP [-] using tg,op versus solar time for the
640
mid-July day and for the three cycles: single-effect H2O/LiBr, single-effect NH3/LiNO3, and
641
NH3/LiNO3 hybrid cycle with pr = 1.5.
M AN U
SC
638 639
AC C
EP
TE D
642
33
ACCEPTED MANUSCRIPT 1.40E+10 1.20E+10 1.00E+10 Qe SE H2O/LiBr 8.00E+09
Qe SE NH3/LiNO3
Qe (J/m2)
Qe hybrid pr = 1.5
6.00E+09
RI PT
Qe hybrid pr = 2 4.00E+09
Qe with tg,op (SE H2O/LiBr and hybrid pr =2) Qe with tg,op SE NH3/LiNO3
2.00E+09
Qe with tg,op hybrid pr =1.5
0.00E+00 40
45
50
55
60
65
70
tg (ºC)
75
80
85
90
95
100
SC
643
Figure 6. Daily solar cold production [J m-2] versus time-constant tg (curves) and tg,op
645
(horizontal lines) for the mid-July day and for the three cycles: single-effect H2O/LiBr,
646
single-effect NH3/LiNO3, and NH3/LiNO3 hybrid cycle with pr = 1.5 and pr = 2.0.
M AN U
644
AC C
EP
TE D
647
34
ACCEPTED MANUSCRIPT 1.20E+10
1.00E+10
8.00E+09 Qe SE H2O/LiBr Qe SE NH3/LiNO3
6.00E+09
Qe hybrid pr = 1.5
Qe (J/m2)
Qe hybrid pr = 2 4.00E+09
RI PT
Qe with tg,op SE H2O/LiBr Qe with tg,op SE NH3/LiNO3 2.00E+09
Qe with tg,op hybrid pr =1.5 Qe with tg,op hybrid pr = 2
0.00E+00 40
45
50
55
60
65
70
tg (ºC)
75
80
85
90
95
100
SC
648
Figure 7. Daily solar cold production [J m-2] versus time-constant tg (curves) and tg,op
650
(horizontal lines) for the mid-September day and for the three cycles: single-effect
651
H2O/LiBr, single-effect NH3/LiNO3, and NH3/LiNO3 hybrid cycle with pr = 1.5 and pr = 2.0.
M AN U
649
652
EP AC C
654
TE D
653
35
ACCEPTED MANUSCRIPT 600
600
500
500 400
400
Qe (W/m2)
Qe (W/m2)
300
300
100
6
10
12
14
Characteristic temperature model
0
16
18
6
8
10
12
14
16
18
solar time (h)
solar time (h)
a-)
b-)
EP
TE D
M AN U
SC
Figure 8. Instantaneous cooling power [W m-2] with tg,op versus solar time in midJuly day. a) H2O/LiBr, b) NH3/LiNO3 for the hybrid cycle with pr = 1.5.
AC C
657 658 659
8
Thermodynamic model
100
Characteristic temperature model
0
655 656
200
Thermodynamic model
RI PT
200
36
ACCEPTED MANUSCRIPT
Highlights: Instantaneous optimum driving temperature tg,op for solar cooling in Madrid. 3 absorption cycles tested: H2O/LiBr and NH3/LiNO3 single effect and hybrid. The tg,op of the hybrid cycle is 16 ºC lower than both single effect cycles. The best fixed driving temperature can reach almost the same behavior than tg,op.
AC C
EP
TE D
M AN U
SC
RI PT
-