Journal of Current Research on Engineering,
Science and Technology
(JoCREST)
ISSN: 2651-2521
Year: 2020
Volume: 6
Issue: 2
doi: 10.26579/jocrest.62
Experimental Investigation of the Effects of Different Adiabatic
Section Lengths on Temperature Distribution in Solar Powered
Gravity Assisted Heat Pipe
Engin ÖZBAŞ
1
& Saba SHABANI
2
Keywords
Heat pipe,
Adiabatic section,
Solar energy.
Abstract
In this study, the effect of the length of the adiabatic section in the gravity
assisted two-phase closed thermosiphon type heat pipe on the heat pipe was
investigated experimentally. For this, four heat pipes with adiabatic zone lengths
of 0cm (a), 5cm (b), 10cm (c) and 15cm (d) were manufactured. Pure water was
used as the working fluid in a, b, c and d heat pipes of the same material and
diameter. Heat pipes were actuated under the same time and conditions with solar
energy in autumn and compared experimentally. The highest condenser
temperatures for a, b, c and d heat pipes were 96.6oC, 74.5oC, 79.8oC and
84.8oC, respectively, in the experiments. While the highest condenser
temperature was reached in (a) heat pipe where there is no adiabatic zone, the
heat pipe with the longest adiabatic zone (d) ranked second.
Article History
Received
28 Nov, 2020
Accepted
30 Dec, 2020
1. Introduction
The use of renewable energy sources is increasing gradually to contribute to the
increasing personal and social energy need with problems such as environmental
pollution and global warming. Solar energy, which is one of the renewable energy
sources, has many applications. As in every system, additional systems can be used
to save energy and increase efficiency in solar energy systems. One of these
additional systems is the heat pipe (Özbaş, 2019: 22). When the literature is
examined, it is seen that there are with wick, without wick, flat plate, loop and
pulsating type heat pipes (Khairnasov and Naumova, 2016: 52). Qu et al,
experimentally investigated heat pipes with adiabatic section shaped as ∩, Ν,
and Ι in their study. For this they manufactured a hybrid flexible oscillating heat
pipes (FOHP) with adiabatic zones made of fluorine rubber material. Deionized
water were used as the working fluid at 50%, 60% and 70% volumetric ratios in
the heat pipes (Qu et al, 2017: 107). Brahim and Jemni investigated the potential
effect of heat pipe adiabatic zone on flow and heat transfer performance of a heat
1
Corresponding Author. ORCID: 0000-0003-4922-7890. Dr, Ondokuz Mayıs University, Yesilyurt
D.C. Vocational School, [email protected]du.tr
2
ORCID: 0000-0001-7483-2254. Master Student, Ondokuz Mayıs University, Graduate School of
Sciences, shaabani.saba@gmail.com
For cited: Özbaş, E. & Shabani, S. (2020). Experimental Investigation of the Effects of Different Adiabatic
Section Lengths on Temperature Distribution in Solar Powered Gravity Assisted Heat Pipe. Journal of Current
Research on Engineering, Science and Technology, 6 (2), 69-78.
Research Article/Araştırma Makalesi
70 Özbaş, E. & Shabani, S. (2020). Experimental Investigation of the Effects of Different
Adiabatic Section Lengths on Temperature Distribution in Solar Powered Gravity
Assisted Heat Pipe
pipe under varying evaporator and condenser conditions. The boundary and
inertia effects of the porous fluid were investigated by the Darcy-Brinkman-
Forchheimer model. A FORTRAN code was developed for the solution of the model
and it was observed that a phase change may occur in the adiabatic region due to
the temperature gradient formed in the porous structure (Brahim and Jemni, 2014:
136). Arab et al, the application of pulsating heat pipes (PHPs) in a solar water
heater (SWH) had investigated. An extra long pulsating heat pipe (ELPHP) has
been designed. The condenser and evaporator sections lengths of the
manufactured heat pipe are 0.8m and 0.96m, respectively, while the length of the
adiabatic zone varies between 0.7m and 1.8m. Four different filling ratios were
compared in the experiments. Four different filling ratios were compared in the
experiments (Arab et al, 2012: 42). A new composite heat pipe (CHP) is proposed
by wrapping the adiabatic part of a conventional heat pipe (HP)with a phase
change material (PCM) in the study by Zhuang et al. Thus, it was aimed to combine
the high thermal conductivity of conventional HP with the high thermal storage
capacity of the PCM. The experimental results showed that with CHP, thermal
performance can be increased and thermal shock can be greatly reduced (Zhuang
et al, 2019: 100). By Czajkowski et al; the effect of different filling ratios (FR) and
different adiabatic section lengths working with different working fluids such as
acetone, ethanol and water in the large-scale pulsating heat pipe (PHP) that can
operate with high heating power up to 2kW has been investigated. As a result of
experiments, it has been shown that the length of adiabatic section does not have a
significant effect on PHP performance for a given working fluid. However, it has
been observed that the effect is different according to different working fluids
(Czajkowski et al, 2020: 165). In this study, the effect of different adiabatic zone
lengths on the temperature distribution in the heat pipe in a gravity assisted two-
phase closed thermosiphon type heat pipe was investigated.
2. Experimental Study
2.1. Gravity Assisted Heat Pipe
Heat Pipe (HP) is a two-phase heat transfer device. Heat transfer is made possible
by taking advantage of the latent enthalpy of the working fluid during the change
of step. It is widely used for various heat flux systems for cooling purposes, such as
fuel cells and electronic devices (Nazari et al, 2018: 32; Ramezanizadeh et al, 2018:
272). Gravity assisted two-phase closed thermosiphon type heat pipe is a pipe with
two ends closed filled with working fluid approximately 5-30% of evaporator's
volume and containing both liquid and gas phases of the working fluid at the same
time. (Faghri, 1995: 6).
Journal of Current Research on Engineering, Science and Technology, 2020, 6 (2), 69-78. 71
Fig. 1. Gravity assisted two-phase closed thermosiphon
Physical mechanism of the heat pipe as seen in Fig. 1 consists of three parts: the
evaporator section, the condenser section and the adiabatic section. In the vapor
phase, the working fluid rises from the interior of the pipe with the influence of the
heat it absorbs from the evaporator region and enters the condenser zone. Here
the working fluid, which transforms into a liquid phase by releasing its heat,
descends from the surface of the pipe to the evaporator region in the shape of a
film by the influence of gravity and completes its cycle (Jafari et al, 2016: 53).
2.2. Experimental Setup
Four heat pipes of the same diameter and material type were manufactured. The
length of the evaporator zone of all heat pipes is 30 cm and the length of the
condenser zone is 15 cm. Fig. 2 shows the manufactured heat pipes.
Fig. 2. The heat pipes
The lengths of the adiabatic zones of each are designed as (a) 0cm, (b) 5cm, (c)
10cm and (d) 15cm, respectively. Heat pipe types and temperature measurement
points are given in Fig. 3. Temperature measurements were made from a total of
four locations, from the midpoints of the condenser and adiabatic zones, and from
the two ends of the evaporator zone.
72 Özbaş, E. & Shabani, S. (2020). Experimental Investigation of the Effects of Different
Adiabatic Section Lengths on Temperature Distribution in Solar Powered Gravity
Assisted Heat Pipe
Fig. 3. The heat pipe types and temperature measurement points
The heat pipes whose preparations have been completed for experimental
comparison are shown in Fig. 4. Adiabatic zones of the heat pipes are well
insulated against heat transfer. Since the temperature distribution in the heat
pipes will be examined, the condenser zones are not coated.
Fig. 4. The heat pipes for the experimental comparison
Solar radiation, ambient temperature and wind speed for the experiment day were
taken from the meteorological station in Yesilyurt DC Vocational School. Type K
thermocouple was used for temperature measurements on the test system and
collected with a UDL100 type data logger. The experiments have been made in the
autumn months at GPS coordinates of 41°14′N and 36°26′E (Samsun, Turkey).
Therefore, in order to benefit more from the sun, the inclination angle of the
systems was set as 41°. In Fig. 5, a general view is given from the experimental
setup.
Journal of Current Research on Engineering, Science and Technology, 2020, 6 (2), 69-78. 73
Fig. 5. A general view from the experimental setup
3. Results
The distribution of meteorological data and insolation values as of 15 October
2020 at the time of the analysis of the experiment is shown in Fig. 6.
Fig. 6. The distribution of meteorological data and insolation values
In Figure 7, the temperature distribution of the (a) type heat pipe without
adiabatic zone is given. It is seen that the temperature values of Tevap-1 and
Tevap-2 points are close to each other and are around 100
o
C. The temperature
values of the Tcond point reached around 95
o
C.
74 Özbaş, E. & Shabani, S. (2020). Experimental Investigation of the Effects of Different
Adiabatic Section Lengths on Temperature Distribution in Solar Powered Gravity
Assisted Heat Pipe
Fig. 7. Temperature distribution for (a) type heat pipe
The temperature distribution in the (b) type heat pipe with an adiabatic zone
length of 5cm is as shown in Fig. 8. The temperature of the Tcond point remained
above 70
o
C.
Fig. 8. Temperature distribution for (b) type heat pipe
The distribution of the temperature measurement points of the (c) type heat pipe
with an adiabatic length of 10 cm is indicated in Fig. 9. The temperature values of
the Tcond point in this heat pipe approached 80
o
C.
Journal of Current Research on Engineering, Science and Technology, 2020, 6 (2), 69-78. 75
Fig. 9. Temperature distribution for (c) type heat pipe
In Fig. 10, the temperature distribution on the (d) type heat pipe, which has the
longest adiabatic zone length with 15 cm, is seen. The temperature value of Tcond
point in (d) type heat pipe has reached up to 85
o
C.
Fig. 10. Temperature distribution for (d) type heat pipe
The comparison of the condenser temperature distribution of four heat pipes is
given in Fig. 11. The highest condenser temperature values were reached with (a)
type heat pipe, followed by (d), (c) and (b) type heat pipes, respectively.
76 Özbaş, E. & Shabani, S. (2020). Experimental Investigation of the Effects of Different
Adiabatic Section Lengths on Temperature Distribution in Solar Powered Gravity
Assisted Heat Pipe
Fig. 11. The condenser temperature distribution of a, b, c and d type heat pipes
In Table 1, the insolation values calculated with the hourly meteorological data of
the experiment day are given. Table 2 and Table 3 show the temperature values
measured on a, b, c and d type heat pipes. Experiments were carried out between
11.00-16.00 hours. However, only hourly results are included in the tables.
Table 1. The values of meteorological data and insolation
Time
INSOLATION
Solar Radiation
Ambient Temperature
Wind Speed
(W/m
2
)
(W/m
2
)
(
o
C)
(km/hour)
11:00
406,80
406,80
24,06
7,2
12:00
428,92
440,00
23,86
7,2
13:00
434,26
431,40
23,98
11,5
14:00
424,54
373,60
24,06
10,1
15:00
399,44
275,80
24,04
10,1
16:00
363,30
163,00
23,82
6,5
Table 2. Temperature values of type-a and type-b heat pipes,
o
C
Type-a
Type-b
Time
Tevp-1
Tevp-2
Tcond
Tevp-1
Tevp-2
Tadyb
Tcond
11:00
27,1
27,2
27,2
27,2
27,3
27,1
27,1
12:00
97,8
95,6
86,6
87,2
83,7
82,5
65,9
13:00
100,8
100,0
95,2
93,0
90,1
88,9
74,5
14:00
102,7
100,5
95,6
92,9
89,0
88,0
72,2
15:00
96,6
95,8
90,4
89,3
86,8
85,6
71,8
16:00
89,7
88,1
76,0
85,6
79,7
80,0
59,4
Journal of Current Research on Engineering, Science and Technology, 2020, 6 (2), 69-78. 77
Table 3. Temperature values of type-c and type-d heat pipes,
o
C
Type-c
Type-d
Time
Tevp-1
Tevp-2
Tadyb
Tcond
Tevp-1
Tevp-2
Tadyb
Tcond
11:00
27,3
27,2
27,3
27,3
27,3
27,4
27,3
27,3
12:00
92,9
89,4
88,7
72,3
90,9
87,3
85,4
72,7
13:00
98,7
96,2
94,8
78,0
95,9
95,4
93,3
84,3
14:00
95,2
94,0
94,3
78,7
93,8
94,2
92,1
83,8
15:00
91,6
90,7
90,8
73,1
89,9
89,9
88,1
78,0
16:00
85,1
83,7
84,0
61,3
84,7
82,3
80,6
65,5
In this study, gravity assisted two-phase closed thermosiphon type heat pipes with
different adiabatic zone lengths were investigated. The effect of four different
adiabatic zone lengths as 0cm (a), 5cm (b), 10cm (c) and 15cm (d) on the
temperature distribution on the heat pipe was experimentally compared. The
effect of the length of the adiabatic zone on the heat transfer from the evaporator
zone to the condenser zone was observed under the same conditions and
simultaneously with solar energy. When the temperature distribution on the heat
pipe is examined, it is understood that the heat insulation of the adiabatic region is
provided well. And also when the results are analyzed, it is seen that heat transfer
is very successful in (a) type heat pipe where there is no adiabatic zone. In other
heat pipes, the heat transfer increased with the increase in the length of the
adiabatic zone and the best result was obtained with the (d) type heat pipe. The
heat pipes were run by solar energy. Performance analysis was not made in the
study in which only temperature distribution was examined. A fluid heating can be
done for performance analysis. Since the experiments were carried out in the
autumn, they were made at a tilt angle of 41
o
. The effect of different adiabatic zone
lengths on the heat pipe at different tilt angles can be examined. In the
experimental study, pure water was used as working fluid in heat pipes. These
heat pipes can be experimentally compared with different working fluids such as
nanofluids.
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