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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 123
ENHANCEMENT OF HEAT TRANSFER FROM PLATE FIN HEAT
SINKS
S.D.Ratnakar1
, D.D.Palande2
1
Mechanical Department, M.C.O.E&RC, Nasik, India - 4220105
2
Mechanical Department, M.C.O.E&RC, Nasik, India - 4220105
Abstract
Heat Sinks are an extremely useful component used to lower the maximum temperature of various electronic devices during
operation so as to increase their thermal efficiency and performance. Fins constitute an important and integral component of
sinks. It is a passive cooling technique. Plate fin heat sinks are used in varied applications owing to its low manufacturing cost,
ease of manufacture and its economical way to dissipate unwanted heat. Steady state natural convection is experimentally
investigated for 03 sets of vertically mounted fin heat sinks. Aluminum is used because of its high conductivity. Length and fin
thickness is kept constant at 200 mm and 05 mm respectively. Fin height is successively increased as 10mm, 30mm,
50mm.Aspect Ratio for above three sets is thus 0.05, 0.15 and 0.25 respectively. Effect of varying height, heat input and aspect
ratio, keeping length constant is investigated on heat transfer through the sinks.
Keywords: Heat Sinks, Fins, Natural Convection, Aspect Ratio.
--------------------------------------------------------------------***----------------------------------------------------------------------
ABBREVIATIONS AND SYMBOLS
h - Convection heat transfer coefficient, W/ (m2
K)
A - Area, m2
Nu -Nusselt number
Gr -Grashof number
S - Fin spacing
H -Fin height, mm
N - Number of fins
L - Fin length, mm
W - Fin width, mm
T - Fin thickness, mm
Sopt - Optimum fin spacing, mm
Ra - Rayleigh number
Qin - Power supplied to heater base plate, W
Qc - Total convection heat transfer rate from fins, W
Tavg - Average base plate temperature, 0
C
Tamb - Ambient temperature,0
C
T - Temperature, 0
C
ΔT - Base-to-ambient temperature difference, 0
C
Tf - Film temperature, 0
C
k - Thermal conductivity, W/ (m K)
g - Gravitational acceleration, m/s2
β - Volumetric thermal expansion coefficient, 1/K
σ - Stefan-Boltzmann constant, W/ (m2
K4
)
ν - Kinematic viscosity, m2
/s
α - Thermal diffusivity, m2
/s
ε - Emissivity
Set A - (L=200mm, H=10mm)
Set B - (L=200mm, H=30mm)
Set C - (L=200mm, H=50mm)
1. INTRODUCTION
Heat sink is an object that absorbs and dissipates heat from
another object by thermal contact. Heat sinks find use in
wide range of applications, providing efficient heat
dissipation. Some applications include cooling of electronic
devices, lasers, heat engines and refrigeration. Thermal
energy transfer between two objects rapidly brings first
object into thermal equilibrium with second lowering
temperature of first object thus accomplishing heat sinks
role as a cooling device. If temperature limits exceed a
certain value in above applications it may even lead to total
system failure. Therefore different methods are used by
engineering systems so as to minimize this overheating
problem as much as possible. Fins form one of the easiest
and cheapest ways to dissipate this heat. Owing to low
production costs and high effectiveness, rectangular fins are
the most popular fin type. Vertical orientation of fins is
widely used from a combination of horizontal and vertical
orientation as it is highly effective. Heat dissipation from
fins to surroundings takes place by two modes convection
and radiation. As aluminium is used for fins, it has low
emissivity value hence radiation heat transfer value is low.
So convection heat transfer is dominant mode of heat
transfer from fins. Heat transfer coefficient and surface area
of fins are two important parameters on which rate of heat
dissipation depends. Fluid can be forced to flow over fins
by fans and in this manner heat transfer coefficient ‘h’ can
be increased. But it is costly and requires more volume to
include fan. Surface area can be increased by addition of
more fins. But distance between adjacent fins reduces due
to addition of more fins. This may result in offering
resistance to air flow thereby reducing heat transfer
coefficient.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 124
2. EXPERIMENTATION
Main components include channel, concrete block, base
plate, fin array, plate heater and power mains. Aerated
concrete block 250x200x100 mm, is fixed on frame which
ensures one dimensional heat dissipation. A removable
acrylic sheet is placed on front surface to replace fin arrays.
Base thickness of arrays is kept as 05mm.The heater
consists of nichrome wire wound around thin mica plate
and mica sheet. Rating of heater plate is 250W and 230 V,
AC.05 mm depth is provided on aerated concrete block to
include heater plate. Extruded surface is kept over fin array
for fitting to aerated concrete block. Concrete block has in-
built 04 bolts to tighten fin array over heater plate Thus air
gap between fin array and heater plate is considered to be
negligible. A concrete block has high insulation quality and
temperature resistance.(K≈0.15 W/m k).
Table -1: Set-up Dimensions
Sr.No Component Dimensions(mm)
1 Frame Channel 550x550x550
2 Heater 180×200×5
3 Concrete 250x200x100
Fin configurations are produced on D.R.O milling. The fin
arrays are produced from rectangular bars with dimensions
180x200x60 mm. Fins are integral with base plate of
thickness 05mm and fin thickness is kept constant at 05mm.
Fig -1: Experimental Set-up
Fig -2: Fin Arrays
The fin array specifications are given in the following table
Table 2: Fin Specifications
Sr.
No.
Fin
Length
(mm)
Fin
Width
(mm)
Fin
Thickness
(mm)
Fin Height
(mm)
1 200 180 05 10
2 200 180 05 30
3 200 180 05 50
3. EQUATIONS
(1) Heat Loss by Convection, Qc:
Qc = (heater input) – (heat loss by radiation, Qr)
Qc = h A ΔT.
Qr = ε σ At (Tavg
4
– Tamb
4
)
(2).Average Heat Transfer Coefficient.
havg = Qc/ (A ΔT)
(3)Mean Film Temperature:
Tf = (Tavg + Tamb)/2
(4)Experimental Nusselt Number:
Nuexp= (havg L)/K
Ra = {gβL3
(Tavg – Tamb)} / (αν).
4. EXPERIMENTAL PROCEDURE
Heat inputs can be adjusted by a dimmer stat. The
temperature of heat sink at different locations and ambient
temperatures are recorded at time interval of 30 minutes till
steady state is reached. Generally it takes around 02 hrs to
attain steady state condition. Temperature variation of
around 0.5°C is taken for steady state approximation. Six
thermocouples are used. Five of them are attached to the
base and one is kept suspended inside the channel to record
ambient temperature.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 125
Parameters used for study are as follows:
Heat Input (Qin) :20W, 40W, 60W, 80W, 100W
Base Temperature : T1, T2, T3, T4, T5
Ambient Temperature : T6
5. EMPIRICAL CORELATIONS
Empirical relations are used to validate the vertical
orientation model. Following correlations are considered:
(1)Mc Adam’s correlation:
(2)Churchill and Chu’s first correlation:
(3)Churchill and Chu’s Second correlation:
(4)Churchill and Usagi’s correlation:
6. RESULT ANALYSIS
6.1 Variation of Nusselt Number with Different
Power Input
Figure3 shows variation of Nusselt No. With different
power input for arrays. Figure shows experimental Nusselt
Number with that of calculated from various existing
Equations. Value of Nu number from experimentation is
close to that of from existing equations. Three sets are
plotted for 10, 30, 50 mm height and length of 200mm.
0
10
20
30
40
50
60
70
20 40 60 80 100
NusseltNo.
Power Input
Exp
McAdams
Chur &Chu I
Chur &Chu
II
Chur &Usagi
Chart -1: Nusselt Vs Input Power Set A
0
10
20
30
40
50
60
70
20 40 60 80 100
NusseltNo.
Power Input
Exp
McAdams
Chur&Chu I
Chur&Chu II
Chur&Usagi
Chart -2: Nusselt Vs Input Power SetB
0
10
20
30
40
50
60
20 40 60 80 100
NusseltNo.
Power Input
Exp
McAdams
Chur&Chu I
Chur&Chu II
Chur&Usagi
Chart -3: Nusselt Vs Input Power Set C
6.2 Variation of Convective Heat Transfer with
Different Power Input for Different Fin arrays
Figure 4 shows variation of convective heat transfer with
different power input for various fin arrays. As power input
increases ‘h’ increases for all arrays. Convective heat
transfer ‘h’is more for arrays with small height when length
and input power is constant.
0
2
4
6
8
10
12
20 40 60 80 100
HeatTransferCoefficient
Power Input
200,10
200,30
200,50
Chart -4: Heat Coefficient Vs Input Power
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 126
6.3 Variation of Convective Heat Transfer Rate
with Fin Height for Different Power Input
Convective heat transfer rate from fin arrays increases with
an increase in fin height. As fin height increases total heat
dissipation area also increases. Convective heat transfer rate
is directly related to surface area in contact with air
0
20
40
60
80
100
20 40 60 80 100
ConvectiveHeatTransfer
Power Input
200,10
200,30
200,50
Chart -5: Convective Heat Transfer Vs Input Power
7. CONCLUSION
 Natural convective heat transfer depends on fin height.
 Convective heat transfer rate from fins increases with
an increase in height of fin arrays.
 Experimental Nusselt Number is quite close to the
value obtained from correlation
 With an increase in heat input and temperature
difference, natural convective heat transfer also
increases.
 With an increase in heat input, heat transfer by
radiation mode also correspondingly increases.
 Convective heat transfer increases with aspect ratio for
given power input.
REFERENCES
[1]. Kamal-Eldin Hassan and Salah A. Mohamed, Natural
Convection from Isothermal Flat Surfaces, ht. J. Heat Mass
Transfer. 1970 Vol. 13, pp. 1873-1886. Pergamon Press.
[2]. E. M. Sd L. F. A. Azevedo, Vertical-Channel Natural
Convection Spanning Between the Fully-Developed Limit
and The Single-Plate Boundary-Layer Limit, Int. Journal
Heat Mass Transfer. 1985Vol. 28, No. 10, pp. 1847-1857
[3]. Burak yazicioğlu and Hafit Yüncü, A Correlation for
Optimum Fin Spacing of Vertically-Based Rectangular Fin
Arrays Subjected to Natural Convection Heat Transfer, J. of
Thermal Science and Technology, 2009, ISSN 1300-3615
29, 1, 99-105
[4]. Mehdi Mehrtash, Ilker Tari, A Correlation for Natural
Convection Heat Transfer from Inclined Plate-finned Heat
Sinks, Applied Thermal Engineering 51 2013 1067-1075.
[5]. F.P.Incropera, D.P. DeWitt, Fundamentals of Heat and
Mass Transfer John Wiley & Sons, New York, 1990.
[6]. Y.A.Cengel, Heat and Mass Transfer Tata McGraw
Hill, 2007.
[7]. Burak Yazicioğlu.,Performance of Rectangular Fins on
a Vertical Base in Free Convection Heat Transfer, M.S.
Thesis in Mechanical Engineering, Middle East Technical
University , Ankara2005.
[8]. Kamil Mert Çakar Numerical Investigation of Natural
Convection from Vertical Plate Finned Heat Sinks Middle
East Technical University , June 2009.
BIOGRAPHY
Swapnil Dipak Ratnakar, Completed B.E
Mechanical from SVIT,
Chincholi.Presently pursuing M.E Heat
Power from Matoshri College of
Engineering and Research, Nasik.

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Enhancement of heat transfer from plate fin heat sinks

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 123 ENHANCEMENT OF HEAT TRANSFER FROM PLATE FIN HEAT SINKS S.D.Ratnakar1 , D.D.Palande2 1 Mechanical Department, M.C.O.E&RC, Nasik, India - 4220105 2 Mechanical Department, M.C.O.E&RC, Nasik, India - 4220105 Abstract Heat Sinks are an extremely useful component used to lower the maximum temperature of various electronic devices during operation so as to increase their thermal efficiency and performance. Fins constitute an important and integral component of sinks. It is a passive cooling technique. Plate fin heat sinks are used in varied applications owing to its low manufacturing cost, ease of manufacture and its economical way to dissipate unwanted heat. Steady state natural convection is experimentally investigated for 03 sets of vertically mounted fin heat sinks. Aluminum is used because of its high conductivity. Length and fin thickness is kept constant at 200 mm and 05 mm respectively. Fin height is successively increased as 10mm, 30mm, 50mm.Aspect Ratio for above three sets is thus 0.05, 0.15 and 0.25 respectively. Effect of varying height, heat input and aspect ratio, keeping length constant is investigated on heat transfer through the sinks. Keywords: Heat Sinks, Fins, Natural Convection, Aspect Ratio. --------------------------------------------------------------------***---------------------------------------------------------------------- ABBREVIATIONS AND SYMBOLS h - Convection heat transfer coefficient, W/ (m2 K) A - Area, m2 Nu -Nusselt number Gr -Grashof number S - Fin spacing H -Fin height, mm N - Number of fins L - Fin length, mm W - Fin width, mm T - Fin thickness, mm Sopt - Optimum fin spacing, mm Ra - Rayleigh number Qin - Power supplied to heater base plate, W Qc - Total convection heat transfer rate from fins, W Tavg - Average base plate temperature, 0 C Tamb - Ambient temperature,0 C T - Temperature, 0 C ΔT - Base-to-ambient temperature difference, 0 C Tf - Film temperature, 0 C k - Thermal conductivity, W/ (m K) g - Gravitational acceleration, m/s2 β - Volumetric thermal expansion coefficient, 1/K σ - Stefan-Boltzmann constant, W/ (m2 K4 ) ν - Kinematic viscosity, m2 /s α - Thermal diffusivity, m2 /s ε - Emissivity Set A - (L=200mm, H=10mm) Set B - (L=200mm, H=30mm) Set C - (L=200mm, H=50mm) 1. INTRODUCTION Heat sink is an object that absorbs and dissipates heat from another object by thermal contact. Heat sinks find use in wide range of applications, providing efficient heat dissipation. Some applications include cooling of electronic devices, lasers, heat engines and refrigeration. Thermal energy transfer between two objects rapidly brings first object into thermal equilibrium with second lowering temperature of first object thus accomplishing heat sinks role as a cooling device. If temperature limits exceed a certain value in above applications it may even lead to total system failure. Therefore different methods are used by engineering systems so as to minimize this overheating problem as much as possible. Fins form one of the easiest and cheapest ways to dissipate this heat. Owing to low production costs and high effectiveness, rectangular fins are the most popular fin type. Vertical orientation of fins is widely used from a combination of horizontal and vertical orientation as it is highly effective. Heat dissipation from fins to surroundings takes place by two modes convection and radiation. As aluminium is used for fins, it has low emissivity value hence radiation heat transfer value is low. So convection heat transfer is dominant mode of heat transfer from fins. Heat transfer coefficient and surface area of fins are two important parameters on which rate of heat dissipation depends. Fluid can be forced to flow over fins by fans and in this manner heat transfer coefficient ‘h’ can be increased. But it is costly and requires more volume to include fan. Surface area can be increased by addition of more fins. But distance between adjacent fins reduces due to addition of more fins. This may result in offering resistance to air flow thereby reducing heat transfer coefficient.
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 124 2. EXPERIMENTATION Main components include channel, concrete block, base plate, fin array, plate heater and power mains. Aerated concrete block 250x200x100 mm, is fixed on frame which ensures one dimensional heat dissipation. A removable acrylic sheet is placed on front surface to replace fin arrays. Base thickness of arrays is kept as 05mm.The heater consists of nichrome wire wound around thin mica plate and mica sheet. Rating of heater plate is 250W and 230 V, AC.05 mm depth is provided on aerated concrete block to include heater plate. Extruded surface is kept over fin array for fitting to aerated concrete block. Concrete block has in- built 04 bolts to tighten fin array over heater plate Thus air gap between fin array and heater plate is considered to be negligible. A concrete block has high insulation quality and temperature resistance.(K≈0.15 W/m k). Table -1: Set-up Dimensions Sr.No Component Dimensions(mm) 1 Frame Channel 550x550x550 2 Heater 180×200×5 3 Concrete 250x200x100 Fin configurations are produced on D.R.O milling. The fin arrays are produced from rectangular bars with dimensions 180x200x60 mm. Fins are integral with base plate of thickness 05mm and fin thickness is kept constant at 05mm. Fig -1: Experimental Set-up Fig -2: Fin Arrays The fin array specifications are given in the following table Table 2: Fin Specifications Sr. No. Fin Length (mm) Fin Width (mm) Fin Thickness (mm) Fin Height (mm) 1 200 180 05 10 2 200 180 05 30 3 200 180 05 50 3. EQUATIONS (1) Heat Loss by Convection, Qc: Qc = (heater input) – (heat loss by radiation, Qr) Qc = h A ΔT. Qr = ε σ At (Tavg 4 – Tamb 4 ) (2).Average Heat Transfer Coefficient. havg = Qc/ (A ΔT) (3)Mean Film Temperature: Tf = (Tavg + Tamb)/2 (4)Experimental Nusselt Number: Nuexp= (havg L)/K Ra = {gβL3 (Tavg – Tamb)} / (αν). 4. EXPERIMENTAL PROCEDURE Heat inputs can be adjusted by a dimmer stat. The temperature of heat sink at different locations and ambient temperatures are recorded at time interval of 30 minutes till steady state is reached. Generally it takes around 02 hrs to attain steady state condition. Temperature variation of around 0.5°C is taken for steady state approximation. Six thermocouples are used. Five of them are attached to the base and one is kept suspended inside the channel to record ambient temperature.
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 125 Parameters used for study are as follows: Heat Input (Qin) :20W, 40W, 60W, 80W, 100W Base Temperature : T1, T2, T3, T4, T5 Ambient Temperature : T6 5. EMPIRICAL CORELATIONS Empirical relations are used to validate the vertical orientation model. Following correlations are considered: (1)Mc Adam’s correlation: (2)Churchill and Chu’s first correlation: (3)Churchill and Chu’s Second correlation: (4)Churchill and Usagi’s correlation: 6. RESULT ANALYSIS 6.1 Variation of Nusselt Number with Different Power Input Figure3 shows variation of Nusselt No. With different power input for arrays. Figure shows experimental Nusselt Number with that of calculated from various existing Equations. Value of Nu number from experimentation is close to that of from existing equations. Three sets are plotted for 10, 30, 50 mm height and length of 200mm. 0 10 20 30 40 50 60 70 20 40 60 80 100 NusseltNo. Power Input Exp McAdams Chur &Chu I Chur &Chu II Chur &Usagi Chart -1: Nusselt Vs Input Power Set A 0 10 20 30 40 50 60 70 20 40 60 80 100 NusseltNo. Power Input Exp McAdams Chur&Chu I Chur&Chu II Chur&Usagi Chart -2: Nusselt Vs Input Power SetB 0 10 20 30 40 50 60 20 40 60 80 100 NusseltNo. Power Input Exp McAdams Chur&Chu I Chur&Chu II Chur&Usagi Chart -3: Nusselt Vs Input Power Set C 6.2 Variation of Convective Heat Transfer with Different Power Input for Different Fin arrays Figure 4 shows variation of convective heat transfer with different power input for various fin arrays. As power input increases ‘h’ increases for all arrays. Convective heat transfer ‘h’is more for arrays with small height when length and input power is constant. 0 2 4 6 8 10 12 20 40 60 80 100 HeatTransferCoefficient Power Input 200,10 200,30 200,50 Chart -4: Heat Coefficient Vs Input Power
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 05 | May-2015, Available @ http://www.ijret.org 126 6.3 Variation of Convective Heat Transfer Rate with Fin Height for Different Power Input Convective heat transfer rate from fin arrays increases with an increase in fin height. As fin height increases total heat dissipation area also increases. Convective heat transfer rate is directly related to surface area in contact with air 0 20 40 60 80 100 20 40 60 80 100 ConvectiveHeatTransfer Power Input 200,10 200,30 200,50 Chart -5: Convective Heat Transfer Vs Input Power 7. CONCLUSION  Natural convective heat transfer depends on fin height.  Convective heat transfer rate from fins increases with an increase in height of fin arrays.  Experimental Nusselt Number is quite close to the value obtained from correlation  With an increase in heat input and temperature difference, natural convective heat transfer also increases.  With an increase in heat input, heat transfer by radiation mode also correspondingly increases.  Convective heat transfer increases with aspect ratio for given power input. REFERENCES [1]. Kamal-Eldin Hassan and Salah A. Mohamed, Natural Convection from Isothermal Flat Surfaces, ht. J. Heat Mass Transfer. 1970 Vol. 13, pp. 1873-1886. Pergamon Press. [2]. E. M. Sd L. F. A. Azevedo, Vertical-Channel Natural Convection Spanning Between the Fully-Developed Limit and The Single-Plate Boundary-Layer Limit, Int. Journal Heat Mass Transfer. 1985Vol. 28, No. 10, pp. 1847-1857 [3]. Burak yazicioğlu and Hafit Yüncü, A Correlation for Optimum Fin Spacing of Vertically-Based Rectangular Fin Arrays Subjected to Natural Convection Heat Transfer, J. of Thermal Science and Technology, 2009, ISSN 1300-3615 29, 1, 99-105 [4]. Mehdi Mehrtash, Ilker Tari, A Correlation for Natural Convection Heat Transfer from Inclined Plate-finned Heat Sinks, Applied Thermal Engineering 51 2013 1067-1075. [5]. F.P.Incropera, D.P. DeWitt, Fundamentals of Heat and Mass Transfer John Wiley & Sons, New York, 1990. [6]. Y.A.Cengel, Heat and Mass Transfer Tata McGraw Hill, 2007. [7]. Burak Yazicioğlu.,Performance of Rectangular Fins on a Vertical Base in Free Convection Heat Transfer, M.S. Thesis in Mechanical Engineering, Middle East Technical University , Ankara2005. [8]. Kamil Mert Çakar Numerical Investigation of Natural Convection from Vertical Plate Finned Heat Sinks Middle East Technical University , June 2009. BIOGRAPHY Swapnil Dipak Ratnakar, Completed B.E Mechanical from SVIT, Chincholi.Presently pursuing M.E Heat Power from Matoshri College of Engineering and Research, Nasik.