Proceedings of REHVA Annual Conference 2015 “Advanced HVAC and Natural Gas Technologies”
Riga, Latvia, May 6 – 9, 2015
                                  Air Heating Solar Collector
                                       for Hemp Drying
                                Ilze Pelēce1, Semjons Ivanovs2, Ādolfs Ruciņš3, Oskars Valainis4
                    1,4
                          Latvia University of Agriculture, 2,3Research Institute of Agricultural Machinery
   Abstract – Attempts to use solar energy for drying of hemp (and                       II. MATERIALS AND METHODS
other agricultural production) have been made in this work. Air is
heated in solar collector approximately to 40 – 60 degrees Celsius,       New construction of solar collector – cylindrical solar
which also results in decreasing of the humidity of this air from 60    collector (Fig. 1) has been investigated.
% (normal ambient air humidity) to 18 - 8 % respectively. Then
such hot dry air is used for drying of hemp or other agricultural
production.
   A new construction of air heating solar collector – a cylindrical
solar collector has been worked out.
  Keywords – Air heating, production drying, solar collector, solar
energy
                          I. INTRODUCTION
   Along with the decrease of the reserves of fossil fuels, as well
as the increasing impact of the use of fossil fuels on the climate,
on the world scale more attention has been paid to renewable
sources of energy, including solar energy.
   In Latvia, solar energy is also used, mostly in solar collectors
for hot water production [1], [2]. Another possible use of solar
energy in Latvia is for drying of agricultural production. Mainly                         Fig. 1. Cylindrical solar collector.
air heating solar collectors have been used for this purpose.
However, due to geographical and climatic conditions in Latvia             It consists of two cylinders: inner is black-painted metal
there are some specific features in comparison with traditional         (galvanized 0.5 mm thick steel sheet, coated with black mat
solar energy using countries [3], [4]. Therefore, traditional flat      silicon color), and outer is transparent 1 mm thick PET material,
plate solar collectors are not efficient enough in Latvia and new       coated with UV-protective film. Diameter of the inner cylinder
constructions of solar collectors must be investigated. One of          is 0.59 m, of the outer 0.67 m, the length of both cylinders is
such new constructions can be a cylindrical solar collector, i.e.       1.3 m. Both cylinders are mounted on one axis, which has been
a solar collector with cylindrical absorber. The main advantage         pointed to the Polar Star to ensure perpendicular striking of
of such construction is the capability to receive solar energy          solar beams to collector surface throughout the entire day. Ends
from all sides, which means to receive also diffused radiation          of cylinders are closed with metal discs, from inside covered
and the radiation reflected from clouds, it is also better in           with 3 cm thick Rockwool heat insulation. There are openings
comparison with the flat plate collector with regard to receiving       in the discs for the inflow of cold air and outflow of the heated
energy in the morning and evening. Similar constructions of             air. These openings are positioned so that inflow is from the
air-heating cylindrical solar collector for drying of agricultural      bottom of the lower end of the cylinder and outflow is at the top
production have already been investigated by other authors [5],         of the upper end of the cylinder. Such positions allow
[6]. But in these investigations a cylindrical solar collector was      convection-provided flow of the air without fan. There are two
placed vertically, and energy output and effectiveness of the           openings in every end allowing using the heated air both from
collector were not investigated, taking only temperature                the inner cylinder and from the space between the metallic
measurements.                                                           cylinder and the transparent one, either together or separately.
   In our work, a new construction of solar collector –                    Temperatures were registered using HOBO logger (Fig. 2).
cylindrical solar collector mounted on the axis pointed to the          This logger is capable to measure air temperature and relative
Polar Star – has been investigated. Continuous measurements             humidity and two external temperatures using sensors
of temperature of the outflowing air allow determining the daily        connected with cables. We used two loggers of that kind to
course of temperature and its dependence on meteorological              measure ambient air temperature and relative humidity, inflow
conditions, and calculating energy output and effectiveness (as         air temperature, outflow air temperature and relative humidity
defined in our previous works, e.g. [7]) of the collector.              and temperature inside the cylinder and in space between the
   In this work, mainly the same collector has been investigated;       cylinder and outer transparent cover.
its use in hemp drying will be considered later.
 doi: 10.7250/rehvaconf.2015.032                                      217
               Proceedings of REHVA Annual Conference 2015 “Advanced HVAC and Natural Gas Technologies”
                                             Riga, Latvia, May 6 – 9, 2015
                                                                                     Fig. 5. 97W flexible PV module.
                                                                   Energy outcome Q(J) from the solar collector has been
           Fig. 2. Temperature and air humidity logger HOBO.     calculated by (1):
  Solar energy was measured using pyranometer CMP 6 from                                 𝑄 = 𝑐 ∙ 𝑚 ∙ ∆𝑇,                       (1)
“Kipp&Zonen”(Fig. 3), corresponding to 1-st class of ISO.
Global solar energy was registered after every 5 minutes.        where c is specific heat of the air, J kg-1 K-1; m is mass of the
                                                                 heated air, kg; ΔT is the difference between inflow and outflow
                                                                 air temperatures, K. The specific heat of air is calculated from
                                                                 (2)
                                                                                               i2 R
                                                                                          c       ,                          (2)
                                                                                                2 
                                                                 where i is number of degrees of freedom, R is universal gas
                                                                 constant, J K-1; µ is molecular mass, kg. The mass of heated air
                                                                 by (3) can be calculated
                                                                                                  pV
                                                                                           m         ,                        (3)
                                                                                                  RT
                    Fig. 3. Pyranometer CMP 6.
                                                                 where p is atmospheric pressure, Pa; V is the volume of the
  Analysis of solar radiation data also gives a view on          heated air, m3; T is air temperature, K. Volume of the heated air
nebulosity.                                                      can be obtained by multiplying velocity of the air flow with
  Air flow was measured using anemometer (Fig. 4)                cross-sectional area of inflow (or outflow) tube of the collector.
                                                                    Calculating in a similar way the energy amount received by
                                                                 water vapor at such little relative humidity of air gives
                                                                 approximately 100 times smaller value than that of the air and
                                                                 therefore can be neglected.
                                                                    The obtained data are compared with theoretical calculations
                                                                 using methods explained in our previous works [7].
                                                                                  III. RESULTS AND DISCUSSION
                                                                     A. Daily course of collector’s temperature
                         Fig. 4. Anemometer.
                                                                   As it was expected, the cylindrical solar collector receives
                                                                 solar energy longer during the day rather than the flat one.
   Measurements have been carried out with and without forced    Theoretically calculated daily course of power of cylindrical (a)
flow. Without forced flow it is convectional flow. For full      and flat (b) solar collectors is shown in Fig. 6.
autonomy of the drying process the forced flow is ensured with
fan powered by a solar cell. The fan with 12 V direct current
electrical engine was used. This voltage was ensured using 97W
flexible PV module (Fig. 5).
                                                               218
                                Proceedings of REHVA Annual Conference 2015 “Advanced HVAC and Natural Gas Technologies”
                                                              Riga, Latvia, May 6 – 9, 2015
                                                                                                  From this picture it can be seen that in the afternoon global
                                                                                               solar energy (curve c) significantly reduces from time to time,
                       1200                                                                    which indicates the presence of clouds, but temperatures of the
                                            a                                                  collector (both inner cylinder and middle space) decrease only
                       1000                                                                    slightly.
                                                                                                  Another interesting fact to be observed in this picture (Fig.
        Power, W m-2
                        800                                                                    8) is that when clouds appear, solar energy among the clouds is
                                                                                               higher than that of the clear day. It means that we receive not
                        600                                                                    only direct radiation, but also reflected from the clouds, which,
                                                            b
                                                                                               in general, moves in other direction than the direct one.
                        400                                                                    Therefore, the cylindrical solar collector, which receives energy
                                                                                               from all sides, has advantages in comparison with the flat one.
                        200                                                                       It might seem that the capability to receive radiation from all
                                                                                               sides, when really radiation comes only from one side at the
                             0
                                                                                               time, will result in large temperature difference between sun
                             00:00       06:00     12:00   18:00   00:00
                                                   Time                                        side and the dark side, but infrared pictures show that it is not
Fig. 6. Theoretically calculated daily course of power of cylindrical (a) and flat             so. Investigations show that at temperature of outgoing air 80⁰C
(b) solar collectors.                                                                          temperature difference of several places of collector surface
                                                                                               does not exceed 10⁰C, such difference is too small to show in
   At midday the amount of received energy is the same for both                                grayscale pictures.
(with equal area), but in the morning and evening the cylindrical
collector receives more energy than the flat one, and it starts to                                 B. Effectiveness
receive the energy earlier in the morning and ends later in the                                   Effectiveness of solar collector is defined [7] as ratio of
evening. Such situation has been observed                                                      energy output from the collector to global solar energy on
                       100                                         1000                        horizontal surface of the same area as the collector has. It is not
                                                                                               the efficiency that is usually used for characterizing solar
     Temperature, ºC
                                                                           Solar energy, W
                        80                                         800                         collectors. Efficiency is the ratio of energy output to solar
                        60                                         600                         energy received by the collector. It does not depend on
                                     a                                                         positioning of the collector, but effectiveness does.
                        40                                         400
                                                                                               Furthermore, solar energy received of the collector is hard to
                        20                            b            200                         evaluate. Global solar energy on the horizontal surface can be
                         0                                         0                           directly measured by pyranometer, but for the calculation of
                         03:00           09:00     15:00   21:00                               energy received by a slope surface solar coordinates must be
                                                 Time                                          known as well as beam and diffused radiation separately. In
                                                                                               contrast to efficiency, effectiveness can be greater than one.
                                                                                                  The simplest way to evaluate the effectiveness of the solar
Fig. 7. Daily course of temperature of the air outflowing from the cylindrical
solar collector (a) and global solar energy (b).                                               collector is to plot daily sums of energy output of the collector
                                                                                               via those of global solar energy, then to draw linear trendline
also experimentally. Fig. 7 shows daily course of temperature                                  taking into account that the intercept must be zero, because
of the outflowing air from the cylindrical solar collector (a) in                              when solar energy is zero then also energy output from the
comparison with that of global solar energy (b), at almost sunny                               collector is zero. The slope of this trendline is the effectiveness
day of July 5.                                                                                 of the collector.
   Other interesting fact is that the cylindrical solar collector                                 For calculating the energy outcome of the solar collector, air
works rather well also on a partly cloudy day (Fig. 8).                                        flow was measured. Without fan (convection flow) it was 1±0.7
                                                                                               m/s. With photovoltaic powered fan the flow was 3.9±0.5 m/s.
                                                                                               Then calculations show the power of the collector 100 – 200 W
                                                                                               on a medium cloudy day without fan and 600 – 1100 W with
                                                                                               the fan. It means that convectional flow without fan is not strong
                                                                                               enough for the effective use of such solar collector, but with the
                                                                                               fan the power of the cylindrical solar collector is sufficient for
                                                                                               the drying of the agricultural production.
                                                                                                  The plot of the daily sum of collector output energy with
                                                                                               respect to those of the global solar energy on horizontal area
                                                                                               (Fig. 9) without fan for 20-days period gives the slope of the
                                                                                               trendline, i.e. effectiveness 0.26 with determination factor of
Fig. 8. Daily course of temperature of space between the cylinder and
transparent coating (a) and inner cylinder (b), and of global solar energy (c).                the trendline R2 = 0.88. The same plot for the collector with fan
                                                                                               (Fig. 10) gives effectiveness 1.5 with determination factor R2 =
                                                                                             219
                   Proceedings of REHVA Annual Conference 2015 “Advanced HVAC and Natural Gas Technologies”
                                                 Riga, Latvia, May 6 – 9, 2015
0.85 for space between the cylinder and transparent cover (for                                                 ACKNOWLEDGMENT
14-days period) and effectiveness 1.3 with determination factor                      This work is supported by the ESF “Attraction of Human
0.86 for the inner cylinder (measurements of 8-days period).                      Resources to Science (2nd round)” project “Development of the
                                                                                  innovative technologies for the accumulation and
                                                                                  production      of     heating      and      cooling”     No
                                                                                  2013/0064/1DP/1.1.1.2.0/13/APIA/VIAA/050
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Fig. 10. Dependence of the daily sum of energy output from cylindrical solar
collector with the fan on the daily sum of the global solar energy, a – space
between cylinder and outer transparent cover, July 9 to 23, b – inner cylinder,
July 24 to 31.
   Further investigations will be carried out with adding the
reflectors to the cylindrical solar collector, and using it for
hemp drying.
                            IV. CONCLUSIONS
   The power of the cylindrical solar collector with the diameter
0.6 m and length 1.3 m is approximately 600 W on a medium
cloudy day and up to 1100 W on a clear day, using solar energy
(photovoltaic) powered fan. Such power is sufficient for drying
of agricultural production and therefore the cylindrical solar
collector can be used for this purpose in Latvia.
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