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Parameters effecting
solar LFPC
performance
GURUDATH G PRABHU
MTECH I YEAR RET
CONTENTS
• LFPC
• CONSTRUCTION
• VARIOUS PARAMETERS
• KEY INVESTIGATIONS
• CONCLUSION
Saturday, April 16, 2016 2
LFPC (Liquid Flat Plate Collector).
 Most common type of collector.
 Simple in design and constructing.
 Used for domestic water heating applications.
 If the fluid is liquid then it is liquid flat plate collector.
 Usually LFPC are stationery and they do not need any tracking.
Saturday, April 16, 2016 3
Saturday, April 16, 2016 4
VARIOUS PARTS OF LFPC ANDTHEIR CONSTRUCTION
Constructional Features
• Usually rectangular case, open at top side, insulation at sides and bottom.
• Heat transfer fluid flowing through the conduits( headers, tubes) which are
attached over or underneath the absorber plate.
• There is transparent cover closing the face of LFPC.
• LFPC casing is usually made up of wood or aluminium.
• Insulation material is glass wool( due to its stability at high temperatures) and it
is up to 25mm-100mm thick.
• Mineral wool, rock wool is also used as insulation material.
• Absorber generally is made of copper metal due to its high conductivity and is
0.2mm to 0.7mm thick.
Saturday, April 16,
2016 5
Constructional Features(cont’d)
• aluminium , steel is also used as absorber material.
• Absorber is spray painted black, and heat treated to improve bonding with
surface or coated with black metal oxides.(nickel oxide, chromium oxide).
• Conduits are same material that of absorber.
• Tubes are of diameter 10-15mm , they are brazed , soldered or pressure bonded
with absorber plate.
• Headers are of 20-25mm diameter.
• Cover is low ferric oxide toughened glass.
• Glass glazing is 2-5mm thick, gap b/w absorber and cover is 15-30mm.
Saturday, April 16,
2016 6
Saturday, April 16, 2016 7
The thermal performance of a collector can be calculated from a first-
law energy balance. according to the first law of thermodynamics, for
a simple flat-plate collector an instantaneous steady-state energy
balance is[1] :
 Useful energy = energy absorbed – heat loss to
gain (Qu) by the collector surroundings
• Absorbed energy = AC FR S
• Lost energy = AC FR UL (Ti-Ta)
where ;
AC = Collector area, m2
FR = Heat removal factor, unitless
S = Absorbed solar radiation, J/m2
UL = Heat transfer loss coefficient, J/m2 °C
Ti = The mean absorber plate temperature, °C
Ta = The ambient temperature, °C.
Saturday, April 16, 2016 9
Saturday, April 16, 2016 10
Useful gain energy equation
    aiLTRcu TTUGFAQ  
Saturday, April 16, 2016 11
   
T
aiLR
R
Tc
u
i
G
TTUF
F
GA
Q
n

 
 
Tc
ip
i
GA
TTCm
n


0'
THREE LOSS COEFFCIENT
• Top loss coefficient( Covers, upper parts)
• Side loss coefficient( through sides)
• Bottom loss coefficient.(bottom such as insulation)
• TOP HEAT LOSS ACCOUNTS MORETHAN 70% OFTOTAL
LOSS AND IS CONTAINS ABSORPTIVITY, EMISSIVITY,
MATERIALVARIANCE, WIND SPEED ETC .
Saturday, April 16, 2016 12
TOP LOSS COEFFCIENT
Saturday, April 16, 2016 13
As the wind loss coefficient increases,
more amount of heat is dissipated to
atmosphere and consequently lower
efficiency can be expected.
BOTTOM LOSS COEFFCIENT
Saturday, April 16, 2016 14
SIDE LOSS COEFFCIENT
Saturday, April 16, 2016 15
PARAMETERS EFFECTING PERFORMANCE
Heat Transfer System
• Heat from the absorber plate is removed from fluid.
• Usually cool fluid enters and gets heated up and is passed.
• Usually thermosiphon principle is used, otherwise external
pumping may be adopted.
• It also depends on type of fluid used.
• Some fluids used are: Ethanol, Methanol, water, Acetone etc.
• Medium inside the collector.
• Usually air, sometime inert gases are filled.
Saturday, April 16, 2016 16
Selective Surfaces
• Absorber plate surfaces which provides high absorptivity for
incoming solar radiation and low emissivity for outgoing solar
radiation is termed as selective surface.
• Solar radiation lies short wavelength band up to 4micro meter,
while the absorber plate the long wave radiation of wavelength
8.3 micro meter.
• No natural surface has this selective surface radiation
characteristics.
• A successful selective surface can be developed by a thick
metallic oxide base on a metal base.
• A good selective surface will have 0.95 absorptivity , 0.1
emissivity.
Saturday, April 16, 2016 17
Selective Surfaces
Saturday, April 16, 2016 18
Table : Characteristics of absorptive coatings
Number of covers
• To minimize the convection and radiation loss the solar
collector is covered with a transparent glass sheet over a
absorber plate.
• Solar radiation incident on glass passes through it and glass
cover.
• Thus the glass sheet cover reduces the heat loss coefficient up
to 10W/m^2 K.
• It is seen that with two glass covers the heat loss coefficient
was still reduced to 4W/m^2 K.
Saturday, April 16, 2016 19
Number of covers
Saturday, April 16, 2016 20
Table : Charactericts of cover plate materials
Transmissivity Absorptivity Product
Saturday, April 16, 2016 21
S is absorbed radiation and it is equal to:
are the view factors from the
collector to the sky and from the collector to the ground, respectively.
The subscripts b,d, and g represent beam, diffuse, and ground ,
respectively. is transmittance and absorptance product.Rb is
the ratio of beam radiation on the tilted surface to that on a horizantal
surface at any time.
Equation 4.2 Absorbed solar radiation[6].
)2/cos1(),2/cos1(  
 
Spacing
• Spacing between the absorber plate and the cover or
between two covers also influence the performance.
• The operating performance varies with space as well as tilt
and service conditions.
• There is no exact way to express spacing.
• The experiments have revealed that 4cm to 8cm will give
good results.
• Large spacing reduces collector area requirements.
Saturday, April 16, 2016 22
Glazing
• Low iron clear glass of 5 mm thickness is used as glazing panel.
• The experiment was conduction to check
Optimum glazing covers and space.
• 5 mm , 10 mm, 15mm space with 1, 2, 3
Glazing covers
Saturday, April 16, 2016 23
Saturday, April 16, 2016 24
Saturday, April 16, 2016 25
Saturday, April 16, 2016 26
Saturday, April 16, 2016 27
(finandtubeareofsanemalerial)
Saturday, April 16, 2016 28
Geometric Parameters
• Spacing: Lower the gas conductivity, the smaller the volume
required for maximum efficiency.
• Tube thickness: Improvement in efficiency when using 1.0 mm
thick tubes instead of 0.5 mm because of the changed
Reynolds number.
• Helical pipe collector gives higher temperature in hot water
tank.
Saturday, April 16, 2016 29
Materials Used for construction
• Absorber plate material : Low cost galvanized iron as absorber
material can give efficiency comparable to copper.
• Tube and header material : Low cost coated stainless steel tube and
aluminium tube gives same performance as copper.
• Absorber coating material : Higher outlet temperature and higher
efficiency for black chrome followed by the matt black and sol
chrome.
• Working fluid : Acetone gives higher efficiency than methanol and
ethanol. Water gives higher efficiency than methanol.
Saturday, April 16, 2016 30
Other things
• Use of PCM :The temperature of water in PCM filled FPC is much
higher.
• Porous aluminium absorbers : Maximum efficiency for the more
porous and thicker absorber at the highest air mass flow rate, but
at very low air flow rates the absorber porosity shows a reversed
effect.
Saturday, April 16, 2016 31
CONCLUSION
• MAJOR LOSSES OCCUR INTOP LOSS.
• LOT OF SCOPE FOR REDUCING ABSORBER AREA.
• OPTIMUM GLAZINGWILL REDUCE LOSSES.
• BEST INSULATION MATERIAL WILL REDUCE LOSSES.
• SELECTION OF RIGHT MATERIAL WILL GIVE US DRASTIC CHANGE IN
EFFICIENCY.
• Solar energy is free if we do not include the initial cost for
installation and the maintenance.
Saturday, April 16, 2016 32
• PERFORMANCE STUDIES OFTUBULAR FLAT PLATE COLLECTORS"
Md. SakhawatHusain International Centre forTheoretical Physics,Trieste, Italy.
INTERNATIONALCENTRE FORTHEORETICAL PHYSICS
• EVALUATION OF HEAT LOSS COEFFICIENTS IN SOLAR FLAT PLATE COLLECTORS
Y. Raja Sekhar1, K.V. Sharma1 and M. Basaveswara Rao2
1Centre for Energy Studies, J. N.T. U. H. College of Engineering, Kukatpally, Hyderabad, India
2Department of Mechanical Engineering, S.V. I.T, Secunderabad, India
• RENEWABLE ENERGY SOURCES AND EMERGINGTECHNOLOGIES
By D.P. KOTHARI, K. C. SINGAL, RAKESH RANJAN
• Recent investigations in solar flat plate collectors P A Kulkarni1, S P Sabnis2, R Sarangi3
Mechanical, DBIT, Mumbai, India
REFERENCE
Saturday, April 16, 2016 33
Saturday, April 16, 2016 34

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Parameters effecting solar lfpc performance

  • 2. CONTENTS • LFPC • CONSTRUCTION • VARIOUS PARAMETERS • KEY INVESTIGATIONS • CONCLUSION Saturday, April 16, 2016 2
  • 3. LFPC (Liquid Flat Plate Collector).  Most common type of collector.  Simple in design and constructing.  Used for domestic water heating applications.  If the fluid is liquid then it is liquid flat plate collector.  Usually LFPC are stationery and they do not need any tracking. Saturday, April 16, 2016 3
  • 4. Saturday, April 16, 2016 4 VARIOUS PARTS OF LFPC ANDTHEIR CONSTRUCTION
  • 5. Constructional Features • Usually rectangular case, open at top side, insulation at sides and bottom. • Heat transfer fluid flowing through the conduits( headers, tubes) which are attached over or underneath the absorber plate. • There is transparent cover closing the face of LFPC. • LFPC casing is usually made up of wood or aluminium. • Insulation material is glass wool( due to its stability at high temperatures) and it is up to 25mm-100mm thick. • Mineral wool, rock wool is also used as insulation material. • Absorber generally is made of copper metal due to its high conductivity and is 0.2mm to 0.7mm thick. Saturday, April 16, 2016 5
  • 6. Constructional Features(cont’d) • aluminium , steel is also used as absorber material. • Absorber is spray painted black, and heat treated to improve bonding with surface or coated with black metal oxides.(nickel oxide, chromium oxide). • Conduits are same material that of absorber. • Tubes are of diameter 10-15mm , they are brazed , soldered or pressure bonded with absorber plate. • Headers are of 20-25mm diameter. • Cover is low ferric oxide toughened glass. • Glass glazing is 2-5mm thick, gap b/w absorber and cover is 15-30mm. Saturday, April 16, 2016 6
  • 8. The thermal performance of a collector can be calculated from a first- law energy balance. according to the first law of thermodynamics, for a simple flat-plate collector an instantaneous steady-state energy balance is[1] :  Useful energy = energy absorbed – heat loss to gain (Qu) by the collector surroundings
  • 9. • Absorbed energy = AC FR S • Lost energy = AC FR UL (Ti-Ta) where ; AC = Collector area, m2 FR = Heat removal factor, unitless S = Absorbed solar radiation, J/m2 UL = Heat transfer loss coefficient, J/m2 °C Ti = The mean absorber plate temperature, °C Ta = The ambient temperature, °C. Saturday, April 16, 2016 9
  • 10. Saturday, April 16, 2016 10 Useful gain energy equation
  • 11.     aiLTRcu TTUGFAQ   Saturday, April 16, 2016 11     T aiLR R Tc u i G TTUF F GA Q n      Tc ip i GA TTCm n   0'
  • 12. THREE LOSS COEFFCIENT • Top loss coefficient( Covers, upper parts) • Side loss coefficient( through sides) • Bottom loss coefficient.(bottom such as insulation) • TOP HEAT LOSS ACCOUNTS MORETHAN 70% OFTOTAL LOSS AND IS CONTAINS ABSORPTIVITY, EMISSIVITY, MATERIALVARIANCE, WIND SPEED ETC . Saturday, April 16, 2016 12
  • 13. TOP LOSS COEFFCIENT Saturday, April 16, 2016 13 As the wind loss coefficient increases, more amount of heat is dissipated to atmosphere and consequently lower efficiency can be expected.
  • 14. BOTTOM LOSS COEFFCIENT Saturday, April 16, 2016 14
  • 15. SIDE LOSS COEFFCIENT Saturday, April 16, 2016 15
  • 16. PARAMETERS EFFECTING PERFORMANCE Heat Transfer System • Heat from the absorber plate is removed from fluid. • Usually cool fluid enters and gets heated up and is passed. • Usually thermosiphon principle is used, otherwise external pumping may be adopted. • It also depends on type of fluid used. • Some fluids used are: Ethanol, Methanol, water, Acetone etc. • Medium inside the collector. • Usually air, sometime inert gases are filled. Saturday, April 16, 2016 16
  • 17. Selective Surfaces • Absorber plate surfaces which provides high absorptivity for incoming solar radiation and low emissivity for outgoing solar radiation is termed as selective surface. • Solar radiation lies short wavelength band up to 4micro meter, while the absorber plate the long wave radiation of wavelength 8.3 micro meter. • No natural surface has this selective surface radiation characteristics. • A successful selective surface can be developed by a thick metallic oxide base on a metal base. • A good selective surface will have 0.95 absorptivity , 0.1 emissivity. Saturday, April 16, 2016 17
  • 18. Selective Surfaces Saturday, April 16, 2016 18 Table : Characteristics of absorptive coatings
  • 19. Number of covers • To minimize the convection and radiation loss the solar collector is covered with a transparent glass sheet over a absorber plate. • Solar radiation incident on glass passes through it and glass cover. • Thus the glass sheet cover reduces the heat loss coefficient up to 10W/m^2 K. • It is seen that with two glass covers the heat loss coefficient was still reduced to 4W/m^2 K. Saturday, April 16, 2016 19
  • 20. Number of covers Saturday, April 16, 2016 20 Table : Charactericts of cover plate materials
  • 21. Transmissivity Absorptivity Product Saturday, April 16, 2016 21 S is absorbed radiation and it is equal to: are the view factors from the collector to the sky and from the collector to the ground, respectively. The subscripts b,d, and g represent beam, diffuse, and ground , respectively. is transmittance and absorptance product.Rb is the ratio of beam radiation on the tilted surface to that on a horizantal surface at any time. Equation 4.2 Absorbed solar radiation[6]. )2/cos1(),2/cos1(    
  • 22. Spacing • Spacing between the absorber plate and the cover or between two covers also influence the performance. • The operating performance varies with space as well as tilt and service conditions. • There is no exact way to express spacing. • The experiments have revealed that 4cm to 8cm will give good results. • Large spacing reduces collector area requirements. Saturday, April 16, 2016 22
  • 23. Glazing • Low iron clear glass of 5 mm thickness is used as glazing panel. • The experiment was conduction to check Optimum glazing covers and space. • 5 mm , 10 mm, 15mm space with 1, 2, 3 Glazing covers Saturday, April 16, 2016 23
  • 27. Saturday, April 16, 2016 27 (finandtubeareofsanemalerial)
  • 29. Geometric Parameters • Spacing: Lower the gas conductivity, the smaller the volume required for maximum efficiency. • Tube thickness: Improvement in efficiency when using 1.0 mm thick tubes instead of 0.5 mm because of the changed Reynolds number. • Helical pipe collector gives higher temperature in hot water tank. Saturday, April 16, 2016 29
  • 30. Materials Used for construction • Absorber plate material : Low cost galvanized iron as absorber material can give efficiency comparable to copper. • Tube and header material : Low cost coated stainless steel tube and aluminium tube gives same performance as copper. • Absorber coating material : Higher outlet temperature and higher efficiency for black chrome followed by the matt black and sol chrome. • Working fluid : Acetone gives higher efficiency than methanol and ethanol. Water gives higher efficiency than methanol. Saturday, April 16, 2016 30
  • 31. Other things • Use of PCM :The temperature of water in PCM filled FPC is much higher. • Porous aluminium absorbers : Maximum efficiency for the more porous and thicker absorber at the highest air mass flow rate, but at very low air flow rates the absorber porosity shows a reversed effect. Saturday, April 16, 2016 31
  • 32. CONCLUSION • MAJOR LOSSES OCCUR INTOP LOSS. • LOT OF SCOPE FOR REDUCING ABSORBER AREA. • OPTIMUM GLAZINGWILL REDUCE LOSSES. • BEST INSULATION MATERIAL WILL REDUCE LOSSES. • SELECTION OF RIGHT MATERIAL WILL GIVE US DRASTIC CHANGE IN EFFICIENCY. • Solar energy is free if we do not include the initial cost for installation and the maintenance. Saturday, April 16, 2016 32
  • 33. • PERFORMANCE STUDIES OFTUBULAR FLAT PLATE COLLECTORS" Md. SakhawatHusain International Centre forTheoretical Physics,Trieste, Italy. INTERNATIONALCENTRE FORTHEORETICAL PHYSICS • EVALUATION OF HEAT LOSS COEFFICIENTS IN SOLAR FLAT PLATE COLLECTORS Y. Raja Sekhar1, K.V. Sharma1 and M. Basaveswara Rao2 1Centre for Energy Studies, J. N.T. U. H. College of Engineering, Kukatpally, Hyderabad, India 2Department of Mechanical Engineering, S.V. I.T, Secunderabad, India • RENEWABLE ENERGY SOURCES AND EMERGINGTECHNOLOGIES By D.P. KOTHARI, K. C. SINGAL, RAKESH RANJAN • Recent investigations in solar flat plate collectors P A Kulkarni1, S P Sabnis2, R Sarangi3 Mechanical, DBIT, Mumbai, India REFERENCE Saturday, April 16, 2016 33