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Solar and Photoenergy Systems

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Received: January 01, 1970 | Published: ,

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Abstract

Solar energy is an alternative source of renewable energy. Conversion of solar radiation into useful heat is the simplest applications of solar energy, which can be used in water heating systems effectively. The most common used device to convert the solar radiation into heat is the flat plate collector. A lot of studies have been conducted to design and analyze the flat plate collector’s thermal behavior and operations and to improve its efficiency. In this work, computational fluid dynamics and finite element method analysis on a flat plat collector were carried out to design and fabricate the low cost solar water heater for rural areas of Oman. The developed prototype delivered100 litres of hot water with an average temperature of 50oC at 6 PM, which is considered as acceptable conditions for smaller families in Oman. Experiments were carried out at different conditions to validate the proposed design and obtained satisfactory results. The experimental results confirmed the validity of boundary conditions used for FEM and CFD analysis. The water outlet temperature of 83oC was observed in the afternoon session and this temperature would be ideal for domestic applications in Oman.

Keywords: solar energy, flat plate collector, fem, cf, oman

Introduction

Today's world is facing many problems with its limited non-renewable energy and global warming. In the last few years (1970-2013) the emission of carbon dioxide in Oman has substantially increased due to the usage of liquid fossils and natural gas.1 Therefore more attention has been focused on another source of energy which is the renewable energy such as solar and wind. In this aspect, Sultanate of Oman government showed initiation on the utilization of solar and wind energy for power generation and domestic applications.2,3

Sultanate of Oman geographical location on the equator helps to develop a hot climate with 300 sunshine days per year make it an ideal location for exploring and utilization of solar energy.3–5 In Oman, some companies can provide devices for houses either for electricity and water heating. However, they don't offer it cheaply and their price not affordable to every Omanis.6–8 Hence, to utilize a significant amount of unused solar energy and also to save the environment from fossil fuel emissions, the proposed work signifies the development of cost-effective solar water heater for rural areas of Oman. Several researchers studied the performance of solar water heaters, and few are discussed in the present work.

Dharmasa3 conducted a cost effective analysis of solar and wind power in Oman concentrating on Photo Voltaic (PV) and Wind Turbine (WT) systems. It was found that combined operation of solar PV and WT systems provided the optimal cost-effectiveness and feasibility.

Jha6 analyzed the estimation and cost of solar PV system and its application in water pumping for a remotely located community in Oman. It was found that initial price of the PV system was higher than a diesel engine. Al-Badi & Albadi7 presented a case study on economic feasibility of installing solar water heater technologies (SWHs) in residential units of Oman. It was found that Oman weather has ideal conditions for installation of SHWs and by using SHWs Oman can save up to 1859 GWh annually. The installation cost of SHWs for the typical residential unit was around 10-year payback period and also, recommended that government should provide subsidies.

Gastli & Charabi8 conducted a case study on solar water heater technologies (SWHs) for saving energy in Oman using RET Screen software. It was found that in Seeb district of Oman annual energy saving is around 335,431MWh and the study results inferred that future industrial applications do not need the construction of additional power plants. The study results highlighted that the government must provide 50% sharing of the capital costto use SWHs in their households. Chaichan2 carried out experiments on in-house developed solar desalination system for Omani families. It produced one to four liters of distilled water for a day. This experiment was part of a program done by Omani Society to raise the importance of using renewable energies in the public and private sectors.

Alvarez9 presented a mathematical model of flat plate collector to study the thermal and hydrodynamic behavior of the collector. 2D and 3D-hydrodynamic and thermal simulation were carried out to determine the thermal efficiency, maximum surface temperature, overall heat loss coefficient and distribution of temperature around the collector. FEM analysis results were validated by experiment. The observed temperature rise of 18.7oC at zero tilt angles and an efficiency of 84.5% was obtained. Also, experimental results highlighted that useful energy transferred to the fluid is 45 W/m at 12:30PM and minimum energy transferred to the fluid is 1 W/m at 5.00 AM. Kazeminejad10 conducted a numerical analysis of parallel flow-flat-plate solar collector with steady-state conduction equation to observe the temperature distribution above the absorber plate. The results revealed that many parameters could affect the performance of flat plate collector, the parameters can be specified as operational, meteorological, environmental parameters; the fluid inlet temperature, tube spacing, and mass flow rate strongly affect the performance of the collector. Rama11 carried out numerical simulations to describe the performance of solar collector; study indicated that two-dimensional model is an excellent tool to optimize the design of flat plate collectors, also mention that flat plate collectors can be designed for any applications which required energy delivery up to 100oC. Experiments were carried out at different localities to validate FEM results. The study results revealed that efficiency at the beginning is increased, and decreased later due to the increase in the ratio of tube spacing to the outer diameter.

Alvarez9 conducted thermal and hydrodynamic modeling of a flat plate collector with the corrugated channel and validated with experiments. Their work highlighted that serpentine geometry gave better performance than parallel one. Sanjay & Dheeraj12 fabricated and studied V-through flat plate collector in hot conditions.13 Their work indicated with the use of low-cost materials, the developed unit could deliver 30L of water at 50oC as an average temperature in comparison to commercially available flat plate collector.14 The study mentioned that reflecting mirror and change of color for the tubes would helped to increase the absorption of heat and thermal efficiency with a minimum loss of energy.15

With this thought, in the present work developed a low cost solar water heater and studied the performance for Oman conditions. CFD and FEM approach was used to finalize the geometry details for the flat plate solar water heater. The proposed set-up could be affordable with lower prices for a rural community in Oman and also signified the efficient utilization of solar energy in Oman.16

Analysis on flat plate collector

Intensity of solar radiation

The placement of earth's orbit around the sun is such that sun-earth distance varies by 1.7 percent and solar radiation outside the earth's atmosphere is nearly of fixed intensity. The radiant energy flux received per second by a surface of unit area held normal to the direction of sun's rays at the mean earth-sun distance is constant throughout the year. This is called as solar constant, ISC and its value is 1367 W/m2. However, the space radiation suffers variation due to the fact that earth rotates around the sun not in a circuital orbit but follows an elliptic path. The intensity of extraterrestrial radiation Iext measured on a plane normal to the radiation on nth day of the year is given in terms of solar constant (Isc):17

I ext = I sc [1+0.033 cos] MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacaWGjbWdamaaBaaajuaibaWdbiaadwgacaWG4bGaamiDaaqc fa4daeqaa8qacqGH9aqpcaWGjbWdamaaBaaajuaibaWdbiaadohaca WGJbaajuaGpaqabaGaai4wa8qacaaIXaGaey4kaSIaaGimaiaac6ca caaIWaGaaG4maiaaiodacaqGGaGaam4yaiaad+gacaWGZbWdaiaac2 faaaa@4ABF@ (1)

In addition, on the basis of transmission coefficients, latitude, declination and hour angle the total received on horizontal surface at ground is calculated from the relation

Itotal = I ext ( τ b + τ d )( cosφ*cosδ*cosω+sinφ*sinδ ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacaWGjbWdamaaBaaajuaibaWdbiaadwgacaWG4bGaamiDaaqc fa4daeqaa8qadaqadaWdaeaapeGaeqiXdq3damaaBaaajuaibaWdbi aadkgaaKqba+aabeaapeGaey4kaSIaeqiXdq3damaaBaaajuaibaWd biaadsgaaKqba+aabeaaa8qacaGLOaGaayzkaaWaaeWaa8aabaWdbi aadogacaWGVbGaam4CaiabeA8aQjaacQcacaWGJbGaam4Baiaadoha cqaH0oazcaGGQaGaam4yaiaad+gacaWGZbGaeqyYdCNaey4kaSIaam 4CaiaadMgacaWGUbGaeqOXdOMaaiOkaiaadohacaWGPbGaamOBaiab es7aKbGaayjkaiaawMcaaaaa@60DB@  (2)

Where, τ is transmission coefficient, φ is latitude angle, δ is declination and ω is hour angle.

Thermal analysis on flat plate collector

In the study of flat plate collector, intensity of solar radiation is represented through Itotal; so the total amount of solar radiation received by the flat plate collector is equal to

Q i =  I total x A MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacaWGrbWdamaaBaaajuaibaWdbiaadMgaaKqba+aabeaapeGa eyypa0JaaeiiaiaadMeapaWaaSbaaKqbGeaapeGaamiDaiaad+gaca WG0bGaamyyaiaadYgaaKqba+aabeaapeGaamiEaiaabccacaWGbbaa aa@4438@ (3)

Where A is area of the collector in m2.

During working conditions, the collector will absorb more heat and its temperature will be higher than surrounding temperature, and heat will be lost to surrounding atmosphere by radiation and convection. The rate of heat loss (Qo) is depending on two factors, the overall heat transfer coefficient (UL) and temperature difference across the collector.18

Q o =  U L A ( T c T a ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacaWGrbWdamaaBaaajuaibaWdbiaad+gaaKqba+aabeaapeGa eyypa0JaaeiiaiaadwfapaWaaSbaaKqbGeaapeGaamitaaqcfa4dae qaa8qacaWGbbGaaeiia8aadaqadaqaa8qacaWGubWdamaaBaaajuai baWdbiaadogaaKqba+aabeaapeGaeyOeI0Iaamiva8aadaWgaaqcfa saa8qacaWGHbaajuaGpaqabaaacaGLOaGaayzkaaaaaa@479C@ (4)

In addition, the rate of useful energy absorbed by the collector is equal to heat taken by water. Hence, useful energy gained by collector is explained as

Q u =  Q i   Q o =m  c f ( T c T i ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacaWGrbWdamaaBaaajuaibaWdbiaadwhaaKqba+aabeaapeGa eyypa0JaaeiiaiaadgfapaWaaSbaaKqbGeaapeGaamyAaaqcfa4dae qaa8qacqGHsislcaqGGaGaamyua8aadaWgaaqcfasaa8qacaWGVbaa juaGpaqabaWdbiabg2da9iaad2gacaqGGaGaam4ya8aadaWgaaqcfa saa8qacaWGMbaajuaGpaqabaWaaeWaaeaapeGaamiva8aadaWgaaqc fasaa8qacaWGJbaajuaGpaqabaWdbiabgkHiTiaadsfapaWaaSbaaK qbGeaapeGaamyAaaqcfa4daeqaaaGaayjkaiaawMcaaaaa@5039@ (5)

The performance of flat plate collector can be measured by the collector efficiency which can be defined as ratio of useful energy gain (QU) to incident solar energy over a period of time

η MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qacqaH3oaAaaa@3851@ = Q u  dt A Idt MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfaieaaaaaa aaa8qadaWcaaWdaeaadaqfGaqabeqabaGaaGzaVdqaa8qacqGHRiI8 aaGaamyua8aadaWgaaqcfasaa8qacaWG1baajuaGpaqabaWdbiaacc kacaWGKbGaamiDaaWdaeaapeGaamyqa8aadaqfGaqabeqabaGaaGza Vdqaa8qacqGHRiI8aaGaamysaiaadsgacaWG0baaaaaa@479F@ (6)

Computational fluid dynamics

CFD analysis is a type of fluid analysis in which specific algorithm and numerical equations are used to solve problems related to fluid flow. In this work, computational fluid dynamics analysis was used to find the pressure drop at designed collectors and also to evaluate the film heat transfer coefficient, h for the flow.19 In CFD, the governing partial differential equations for energy, momentum and mass were solved for steady incompressible flow.20 The velocity-pressure coupling had been done by using SIMPLE algorithm (Semi Implicit Method for Pressure Linked Equation) and the mean flow equations are represented in equations (7),(8) and (9).

For Continuity equation,

ρ t +div(ρu)=0 MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfa4aaSaaae aacqGHciITcqaHbpGCaeaacqGHciITcaWG0baaaiaaysW7cqGHRaWk caaMe8UaamizaiaadMgacaWG2bGaaiikaiabeg8aYjaaysW7caWH1b GaaiykaiaaysW7cqGH9aqpcaaMe8UaaGimaaaa@4D65@ (7)

Momentum equation,

(ρu) t +div(ρuu)= p x +div(μgradu) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfa4aaSaaae aacqGHciITcaGGOaGaeqyWdiNaamyDaiaacMcaaeaacqGHciITcaWG 0baaaiaaysW7cqGHRaWkcaaMe8UaamizaiaadMgacaWG2bGaaiikai abeg8aYjaadwhacaWH1bGaaiykaiaaysW7cqGH9aqpcaaMe8UaeyOe I0YaaSaaaeaacqGHciITcaWGWbaabaGaeyOaIyRaamiEaaaacaaMe8 Uaey4kaSIaaGjbVlaadsgacaWGPbGaamODaiaacIcacqaH8oqBcaaM e8Uaam4zaiaadkhacaWGHbGaamizaiaaysW7caWG1bGaaiykaiaays W7aaa@6756@ (8)

and Energy equation,

(ρE) t +div(ρEu)=pdivu+div(kgradT)+Φ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfa4aaSaaae aacqGHciITcaGGOaGaeqyWdiNaamyraiaacMcaaeaacqGHciITcaWG 0baaaiaaysW7cqGHRaWkcaaMe8UaamizaiaadMgacaWG2bGaaiikai abeg8aYjaadweacaWH1bGaaiykaiaaysW7cqGH9aqpcaaMe8UaeyOe I0IaamiCaiaaygW7caaMe8UaamizaiaadMgacaWG2bGaaGjbVlaahw hacaaMe8Uaey4kaSIaaGjbVlaadsgacaWGPbGaamODaiaacIcacaWG RbGaaGjbVlaadEgacaWGYbGaamyyaiaadsgacaaMe8UaamivaiaacM cacaaMe8Uaey4kaSIaaGjbVlabfA6agjaaysW7aaa@7020@ (9)

Where r density of fluid, u is velocity, µ is viscosity, E is energy, p is pressure, k is thermal conductivity and T is temperature.

Conservation equations were solved in order to yield the velocity and temperature for the fluid (water) flow in the copper tubes.

Finite element analysis

FEM analysis for flat plate collector panel with absorption plate was studied under steady state conditions. Energy balance for the absorption plate can be calculated as

2 T x 2 + 2 T y 2 = U L kt [ T T a I tot U L ] MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfa4aaSaaae aacqGHciITdaahaaqabKqbGeaacaaIYaaaaKqbakaadsfaaeaacqGH ciITcaWG4bWaaWbaaeqajuaibaGaaGOmaaaaaaqcfaOaaGjbVlabgU caRiaaysW7daWcaaqaaiabgkGi2oaaCaaabeqcfasaaiaaikdaaaqc faOaamivaaqaaiabgkGi2kaadMhadaahaaqabKqbGeaacaaIYaaaaa aajuaGcaaMe8Uaeyypa0JaaGjbVpaalaaabaGaamyvamaaBaaajuai baGaamitaaqcfayabaaabaGaam4AaiaadshaaaWaamWaaeaacaWGub GaeyOeI0IaamivamaaBaaajuaibaGaamyyaaqcfayabaGaeyOeI0Ya aSaaaeaacaWGjbWaaSbaaKqbGeaacaWG0bGaam4BaiaadshaaKqbag qaaaqaaiaadwfadaWgaaqcfasaaiaadYeaaKqbagqaaaaaaiaawUfa caGLDbaacaaMe8oaaa@62E5@ (10)

Similarly, useful energy gain in the absorption plate was utilized to heat the water entering the collector, the energy balance equation on the fluid can be represented as

m . C f dT dx + U o 2 ( π D o )( T f T a )= q u (x)2t+ I tot . D o MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqcfa4aaCbiae aacaWGTbaabeqaaiaac6caaaGaam4qamaaBaaajuaibaGaamOzaaqc fayabaWaaSaaaeaacaWGKbGaamivaaqaaiaadsgacaWG4baaaiaays W7cqGHRaWkcaaMe8+aaSaaaeaacaWGvbWaaSbaaKqbGeaacaWGVbaa juaGbeaaaeaacaaIYaaaamaabmaabaGaeqiWdaNaamiramaaBaaaju aibaGaam4BaaqcfayabaaacaGLOaGaayzkaaWaaeWaaeaacaWGubWa aSbaaKqbGeaacaWGMbaajuaGbeaacqGHsislcaWGubWaaSbaaKqbGe aacaWGHbaajuaGbeaaaiaawIcacaGLPaaacaaMe8Uaeyypa0JaaGjb VpaaxacabaGaamyCamaaBaaajuaibaGaamyDaaqcfayabaGaaiikai aadIhacaGGPaGaaGOmaiaadshacqGHRaWkcaWGjbWaaSbaaKqbGeaa caWG0bGaam4BaiaadshaaKqbagqaaaqabeaacaGGUaaaaiaadseada Wgaaqcfasaaiaad+gaaKqbagqaaiaaysW7aaa@6936@ (11)

Where m is mass flow rate of fluid, Uo is overall heat transfer coefficient, Do is outer diameter of tube and t is thickness of tube. Energy balance equations were solved iteratively to obtain the temperature contours across the collector.

Results and discussion

Solar intensity of radiation

The solar intensity calculation had been carried out to determine intensity of solar radiation in Oman. The study highlighted that solar intensity in the summer period is around 1000W/m2. However, experimental study indicated a maximum solar intensity of 1017 W/m2 as shown in Figure 1. In the late evening, this value is reduced to 91 W/m2. Thus, the study gave confidence in solar intensity calculations (Table 1).

Figure 1 Solar intensity Data (Date: April 26, 2016).

Parameter

Values

Collector heat input

1367 W

Heat loss from collector

70 W

Useful energy input to collector

1297 W

Efficiency

56%

Table 1 Thermal analysis results for flat plate solar collector

CFD analysis on flat plate collector

The straight tube and serpentine geometry were considered for the CFD analysis to find the pressure drop at designed collectors and heat transfer coefficient, h for the flow. The modeling part of fluid domain was prepared through Pro-ECAD software and imported to ANSYS-FLUENT platform. In order to predict the accurate pressure drop fine meshing approach was incorporated in the current study. The meshed details are highlighted in Table 2 and meshed geometry is presented in Figure 2.

Figure 2Meshed model of CFD analysis. (A) Straight tubes. (B) Serpentine.

 

Straight pipe

Serpentine

Number of elements

355345

304315

Number of nodes

74963

66002

Mesh type

Tetrahedral – 10 node element

Tetrahedral – 10 node element

Table 2 Mesh details – CFD analysis

Boundary conditions: The accurate boundary conditions plays an important role in CFD analysis. From the entry flow rate, the flow velocity of 0.004 m/s was considered for the simulation and fluid temperature of 303 K was chosen for the current study as highlighted in Table 3.

Type of geometry

Straight

Serpentine

Velocity at inlet point, m/s

0.004123

0.004123

Entry fluid temperature, K

303K

303K

Wall Material

Copper

Copper

Fluid

Water

Water

Table 3 Boundary conditions used for the simulation

CFD results: Figure 3 revealed the pressure drop variation across the straight tubes and serpentine geometries. The study results indicated that in straight tubes geometry the flow enters uniformly in all the tubes and maximum pressure drop of 0.003Pawas noticed at the outlet. The low pressure drop was due to the chosen pipe dimensions of 25.4 mm diameter and 1 m length which did not caused the reverse flow in the flow path. However, serpentine geometry with 5-passes showed pressure drop value of 0.056Pa. This could be due to the fact that, in serpentine arrangement, flow enters through the zigzag path and augments the pressure drop at the outlet. Also, the study results indicated that further increase of the passes in serpentine geometry will be contributing more pressure drop across the flow. Hence, the results clearly indicated that straight tube flow path was better than serpentine geometry.

Figure 3 Contours of pressure drop – Straight tubes and Serpentine geometry. (A) Straight tubes. (B) Serpentine.

Similarly, flow velocity contours for the straight tubes and serpentine geometry are presented in Figure 4. The results indicated that there is no reverse flow in the flow path and uniform flow without eddies was noticed with straight tubes geometry. The maximum flow velocity of 0.03 m/s was noticed with serpentine geometry as against a minimum value of 0.007 m/s with straight tubes. This could be due to the fact that the serpentine geometry will be contributing more pressure drop which indirectly augments the higher outlet velocity of the flow.

Figure 4 Velocity contours for the Straight tubes and Serpentine geometry. (A) Straight tubes. (B) Serpentine.

In addition, CFD analysis gave important information on average film heat transfer coefficient across the flow path. The calculated Nusselt number from the simulations indicated a heat transfer coefficient value of 18 W/m2K with straight tubes geometry. This value was used in FEM analysis for predicting the temperature across the tube.

Finite element analysis

CFD analysis results revealed that straight tube geometry is found to be better for the proposed low cost solar water heating system. Hence, in FEM analysis straight tube geometry was used to simulate the temperature contours across the tube. The proposed collector assembly was modelled through Pro-E and imported to Ansys-Workbench. The meshed details are highlighted in Table 4 and the meshed geometry is indicated in Figure 5.

Figure 5 Flat plate collector assembly- meshed model.

Number of nodes

19016

Number of elements

6082

Mesh type

Tetrahedral 10 node

Table 4 Mesh details – FEM analysis

Boundary conditions:

For accurate prediction of temperature across the collector tubes, the following boundary conditions were used for FEM-thermal analysis, (Table 5).

 

Value

Zone

Heat flux

950 W/m2

Absorption plate

Film heat transfer coefficient

18W/m2K

Tubes

Ambient temperature

35oC

Material

Copper

Tubes

Insulated condition

-

Box, Insulation plate

Table 5 Boundary conditions used for FEM analysis

FEM results: The temperature distributions across the collector tubes is shown in Figure 6. The study results indicated 77oC - 84oC temperature variation across the collector tubes and these temperatures gave information on outlet water temperature from the solar water heater. In straight tubes geometry, all the tubes experienced uniform temperature and the maximum temperature was around 84oC at the flow exit. Thus, FEM thermal analysis coupled with CFD results indicated that five straight tubes will be sufficient to achieve the outlet water temperature of 84oC with minimum pressure drop.

Figure 6 Temperature contours across the tubes.

Experimental set-up: In order to validate the CFD and FEM results, experimental set-up was developed in-house to study the performance of low cost solar water heater. In the proto model development, low cost wooden box, aluminium absorption plate and copper tubes were used. The developed low cost collector was connected to overhead water tank, which is the typical water storage arrangement in Omani houses as shown in Figure 7. In addition, the complete experiment set-up with water flow path is indicated in Figure 8.

Figure 7 Pipe line path inlet to solar water heater.

Figure 8 Experimental set-up of low cost solar water heater.

Experimental results: To study the performance of low cost solar water heater, experiments were carried out in the month of April, 2016. Pyranometer unit was used to record the solar intensity values and two thermometers were mounted at the inlet and outlet of collector to record the water temperatures. For each day, data were collected from 7AM to 6PM to know the behavior of the water heater. The variation of water outlet temperature at different dates is highlighted in Figure 9. On April 24, 2016 the minimum water outlet temperature observed was around 61oC. This could be due to cloudy climatic conditions which led to low solar intensity values. The experimental test results indicated maximum temperature of 83.4oC on April 27, 2016 at 12:00 PM and observed solar intensity value was around 1017W/m2. The experimentally observed outlet water temperature results almost matched with the FEM simulation value of 84.6oC as indicated in Figure 6. It gave confidence to boundary conditions used for CFD and FEM simulations.

Figure 9 Variation of Water outlet temperatures.

In order to experience the seasonal conditions of sun orientation in Oman, experiments were carried out with different tilting angles of collector as represented in Figure 10. The water outlet temperature was recorded for tilting angles of 42o, 66o & 90o on the collector. From Figure 10, it is confirmed that up to 12PM, collector tilting angle of 90o was effective due to maximum concentration of solar radiation on the collector. However in the afternoon sessions around 2PM, 66o tilting angle gave better results than the 90o orientation of the collector. This could be due to orientation of the sun and amount of sun rays dropped on the collector. Thus, this study gave information about tracking of the solar rays on collector surface which would give better performance for the water heating system. However, without a tracking system, 90o tilting angle orientation for the collector was better for water heating in Oman.

Figure 10 Variation of Water outlet temperatures with different tilting angle.

Flat plate collector performance: The measured experiment data were used to evaluate the energy gained by water circulating through heating system. The study showed that the collector performance is directly related to energy taken by water and absorbed solar intensity. It is observed that a collector efficiency of 50~55% for the designed low cost water heater is almost nearer to the value predicted from thermal analysis as represented in Table 6. However, on April 24, 2016, energy gained by water was less due to cloudy weather.

Date

Max. solar intensity, W/m2

Qwater, MJ

ηcollector, %

*April 24

850

2.62

42

*April 25

990

3.55

50

*April 26

1017

3.89

53

*April 27

1030

4.21

55

Table 6 Results of collector performance

 *- Data recorded in the year 2016

Cost comparison

The developed flat plate solar water heater consists of low cost wooden box, aluminium absorption plate, copper tubes and insulation sheets as shown in Table 7. Fabrication of low cost water heater was carried out in-house and its cost was compared with the price of commercial solar water heater available in Oman market. The cost comparison analysis showed that the cost of low cost water heater was at least 70% lower than commercially available solar water heater in Oman. Moreover, the developed low cost water heater delivered 100 litres of water with an average water temperature of 50oC.

 

Dimensions

Wooden Box

1m x 1m x 20 mm

Absorber plate

0.980m x 0.980m x 10mm

Insulation layer

0.980m x 0.980m x 20mm

Pipes (Water entry and exit)

ᶲ50.8 mm x 0.980m

Absorbing pipes

ᶲ25.4 mm x 0.980m

Cost of Low cost of water heater = OMR 90

Cost of Commercial water heater = OMR 160

Table 4 Low cost water heater parts and cost comparison

Conclusion

In the present work, performance of low cost flat plate solar water was studied for Oman conditions. A proto model was developed in-house and produced100 litres of hot water, which is considered as normal consumption of hot water for smaller houses in Oman. CFD and FEM approach was used to finalize the dimensions for solar water heater. The following are the outcomes of the present work:

  1. CFD results indicated that straight absorber tubes geometry is preferable than serpentine configuration.
  2. The experimental results highlighted a maximum water temperature of 83.4oC, which is almost in line with FEM simulated values under steady state conditions.
  3. Tilting angle of 90o is better until 12PM and for afternoon sessions 66o tilting angle showed good results due to orientation of solar radiations on the collector surface. However, in the present set-up solar tracking system was not incorporated and from low cost point of view, 90o tilting angle would be an ideal option for Oman conditions.
  4. Moreover, study results showed the collector efficiency of 50~55%, which is almost equal to efficiency obtained through thermal calculations.
  5. In addition, cost of the developed water heater is at least 70% lower than the commercially available water heater in the market.

Acknowledgements

None.

Conflicts of interest

The authors declare no conflict of interest.

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