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Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17
www.ijera.com 13 | P a g e
Theoretical Convective Heat Transfer Model Developement of
Cold Storage Using Taguchi Analysis.
Dr.N.Mukhopadhyay1
, Suman Debnath2
,
1
Assistant Professor, Department of Mechanical Engineering, Jalpaiguri Government Engineering College
2
Post Graduate Scholar, Department of Mechanical Engineering,Jalpaiguri Government Engineering College,
India.
Abstract
Energy crisis is one of the most important problems the world is facing now-a-days. With the increase of cost of
electrical energy operating cost of cold storage storing is increasing which forces the increased cost price of the
commodities that are kept. In this situation if the maximum heat energy(Q) is absorbed by the evaporator inside
the cold room through convective heat transfer process in terms of –heat transfer due to convection and heat
transfer due to condensation, more energy has to be wasted to maintain the evaporator space at the desired
temperature range of 2- 8 degree centigrade. In this paper we have proposed a theoretical heat transfermodel of
convective heat transfer incold storage using Taguchi L9 orthogonal array. Velocity of air(V), Temperature
difference(dT), RelativeHumidity(RH)are the basic variable and three ranges are taken each of them in the
model development. Graphical interpretations from the model justifies the reality
Keywords: cold storage, convective heat transfer model, heat absorbed by evaporator, Taguchi Analysis.
I. Introduction
Demand for cold storages have been increasing
rapidly over the past couple of decades so that food
commodities can be uniformly supplied all through
the year and food items are prevented from perishing.
India is having a unique geographical position and a
wide range of soil thus producing variety of fruits and
vegetables like apples, grapes, oranges, potatoes,
chilies, ginger, etc. Marine products are also being
produced in large quantities due to large coastal
areas.
The cold storage facilities are the prime
infrastructural component for such perishable
commodities. Besides the role of stabilizing market
prices and evenly distributing both on demand basis
and time basis, the cold storage industry provide
other advantages and benefits to both the farmers and
the consumers. The farmers get the opportunity to get
a good return of their hard work. On the consumer
sides they get the perishable commodities with lower
fluctuation of price.
Very little theoretical and experimental studies
are being reported in the journal on the performance
enhancement of cold storage.
Energy crisis is one of the most important
problems the world is facing nowadays. With the
increase of cost of electrical energy operating cost of
cold storage storing is increasing which forces the
increased cost price of the commodities that are kept.
So it is very important to make cold storage energy
efficient or in the other words reduce its energy
consumption. Thus the storage cost will eventually
comes down. In case of conduction we have to
minimize the leakage of heat through wall but in
convection maximum heat should be absorbed by
refrigerant to create cooling uniformity thought out
the evaporator space.If the desirable heat is not
absorbed by tube or pipe refrigerant then temp of the
refrigerated space will be increased, which not only
hamper the quality of the product which has been
stored there but reduces the overall performance of
the plant. That’s why a mathematical modeling is
absolutely necessary to predict the performance.
In this paper we have proposed a theoretical heat
transfer model of convective heat transfer model
development of a cold storage using Taguchi L9
orthogonal array. Velocity of air (V), Temperature
difference (dT), Relative Humidity (RH)are the
basic variables and three ranges are taken each of
them in the model development. Graphical
interpretations from the model justifies the reality
II. Model development
Relationship between heat gain & energy
consumption is given by
E= (Q t)/COP [M.S.Soylemez, M.Unsal ](1997) [1]
E=energy consumption of refrigeration system
(kw/h), t=equivalent full load hours of operation of
refrigeration system(hrs), COP= co efficient of
performance of refrigeration plant., Q= heat energy
extracted from cold room (Joule)
Response variableis heat transfer due to
convection and condensation and predictor variables
are Velocity of air (V), Temperature difference (dT),
Relative Humidity (RH) .With the help of Taguchi
methodology we construct our design matrix.
RESEARCH ARTICLE OPEN ACCESS
Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17
www.ijera.com 14 | P a g e
Orthogonal arrays provide a best set of well
balanced (minimum) experiments .It was developed
by C.R.Rao (1947) Popularized by Gene chi Taguchi
(1987).The number of rows of an orthogonal array
represents the requisite number of experiments.
III. Regression analysis
Regression analysis is the relationship between
various variables. By regression analysis one can
construct a relationship between response variable
and predictor variable. It demonstrates what will be
the changes in response variable because of the
changes in predictor variable. Simple regression
equation is
y=a+ b x
In this problem more than one predictor variable
is involved and hence simple regression analysis can
not be used. We have to take the help of multiple
regression analysis. There are two types of multiple
regression analysis- 1) Simple multiple regression
analysis (regression equation of first order) 2)
Polynomial multiple regression analysis (regression
equation of second order or more)
Simple multiple regression analysis is represented by
the equation of first order regression
Y= β0+β1X1+β2X2+β3X3+…………………..+ε
Where β is constant terms & X is the variables &
ε is the experimental error.
Polynomial multiple regression analysis equation
is
Y = β0+ β1X1+β2X2+β3X3+ β 11X2
11+ β 22X2
22+
β33X2
33+ β12X1X2+ β13X1X3+ β23X2X3
The above equation is second order polynomial
equation for 3 variables. Where β are constant, X1 ,
X2 , X3 are the linear terms, X12 X13 X23 are the
interaction terms between the factors, and lastly X11
X22 X33 are the square terms.
Q (heat due to conv+condensation) = response variable, V, dT,
RH= predictor variable.
Polynomial regression equation becomes after
replacing real problem variables
Q (heat due to conv+condensation) = β0+β1(V)+β2 (dT)+β3
(RH)+ β 11 (V)*(V)+ β 22(dT)*(dT)+β33 (RH)*(RH)+
β12(V)*(dT)+ β13(dT)*(RH)+ β23(RH)*(V)
To solve this equation following matrix method is
used
Y= [β][ X ]
[β]=Y [X-1
] where [β] is the coefficient matrix, Y is
the response variable matrix; [X-1] is the inverse of
predictor variable matrix.
In this problem there are 3 independent variables and
each variable has 3 levels and hence from the
Taguchi Orthogonal Array (OA) table L9 OA is best
selected.
Cold storage Description
The overall dimensions of cold storage plant are
87.5mx34.15mx16.77m.The cold storage building is
of five floors with each floor having 2 cold chambers
of 43.25m x 17m sizes operating at different
temperature as per the requirements of commodities.
For our analysis purpose we only considered zone 1
which is referred as cold room.
IV. Parameter &Range Selection
The one chamber of cold storage Length ,Breath
and Height 87.5m,34.15m and 16.77m respectively.
The three values of air velocity(V) of evaporator
space are 0.74m/s, 1.25m/s and 1.76m/s respectively.
The three values of temperature difference (dT) of
evaporator space are 2, 5 & 8 centigrade respectively.
The three values of relative humidity (RH) of
evaporative space are 0.85, 0.90 & 0.95 respectively.
V. Heat (heat due to conv+condensation)
Calculation
In this study heat transfer from evaporating space
to refrigerant (which are in tube or pipe) only being
considered. The transfer heat evaporating space to
refrigerant are calculated in terms of velocity of air
(V), temp. difference (dT) & relative humidity RH) .
Only convection heat transfer effect is being
considered in this study.
Basic equation for heat transfer
QT = Qconv+ Qcondensation.
Qconv=AhcdT&Qcondensation=Ahm(RH)hfg.
Here Qconv=heat transfer due to convection
&Qcondensation=heat transfer due to condensation &
QT=Total heat transfer or absorb heat into refrigerant
.
And hc/hm=cp(Le)2/3
&hcL/K=Nu=0.026(Re)0.8
(Pr)0.3
The final heat transfer equation due to velocity of air
(V), temp. difference (dT) & relative humidity RH)
is QT=7.905V0.8
(dT + 2490 RH).
Hera A=surface area of tubes in evaporator space
1872 m2
.hc=convective heat transfer co-efficient.
hm=convective mass transfer co-efficient.hfg=latent
heat of condensation of moisture 2490 KJ/Kg-K.
Cp=specific heat of air 1.005 KJ/Kg-K. Le=Lewis
number for air it is one.
After getting the full observation table which include
all the predictor variables and response variable,
values can be computed easily in the following
equation-
Q (heat due to conv+condensation) = β0+β1(V)+β2 (dT)+β3
(RH)+ β 11 (V)*(V)+ β 22(dT)*(dT)+β33 (RH)*(RH)+
β12(V)*(dT)+ β13(dT)*(RH)+ β23(RH)*(V)
We get nineequations but number of unknowns
are ten. Now we can solvethese equations-eliminate
some of variables in terms of others. Then we get[ X
] matrix as [9*9]. We also get response variable
matrix [Q] which is a [9*1] matrix. With the help of
following equation we can get the co efficient values-
[β]=[Q]*[X-1
] where [x]-denotes the variable matrix.
The proposed theoretical mathematical model for
heat transfer in cold storage is –
Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17
www.ijera.com 15 | P a g e
Q (heat due to conv+condensation) = -770+2791(V)-
34(dT)+2791(RH)-1143(V)*(V)-
1(dT)*(dT)+772(RH)*(RH)+ 9(V)*(dT)+
46(dT)*(RH)+ 15230(RH)*(V) .
VI. Results and Discussions
L9 OA combination Table with notation for Matrix design-
L9 table with various factors level
TABLE 1 TABLE 2
Levels Velocity
of air
(V)(m/s)
Temperature
difference(dT)(c
entrigade)
Relative
humidity
1 0.74 2 0.85
2 1.25 5 0.90
3 1.76 8 0.95
Observation table
TABLE 3
Obs no - V dT RH Q
1 0.74 2 0.85 13162.61
2 0.74 5 0.90 13954.63
3 0.74 8 0.95 14746.05
4 1.25 2 0.90 21196.58
5 1.25 5 0.95 22401.23
6 1.25 8 0.85 20075.48
7 1.76 2 0.95 29416.29
8 1.76 5 0.85 26359.37
9 1.76 8 0.90 27944.56
V dT RH
0.74 2 0.85
0.74 5 0.90
0.74 8 0.95
1.25 2 0.90
1.25 5 0.95
1.25 8 0.85
1.76 2 0.95
1.76 5 0.85
1.76 8 0.90
Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17
www.ijera.com 16 | P a g e
Figure 1: variation of heat transfer with air velocity.
Figure 1 shows that heat absorption increase with velocity of air increases .
Figure 2 : variation of heat transfer with temperature difference.
Figure 2 shows that heat absorption increase with temperature difference increase and at lower temperature
difference it is more effected than the higher temperature difference.
Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17
www.ijera.com 17 | P a g e
Figure 3 : variation of heat transfer with relative humidity.
Figure 3 shows that heatabsorption increase with
increase in relative humidity but in this case gradient
is higher than the figure 2 case.
VII. Conclusion
1.with increasing the velocity of air ,temperature
difference and relative humidity heat absorb by the
refrigerant is increased.
2.To create maximum cooling effects maximum heat
transfer is required at the values of air velocity,
temperature difference and relative humidity are 1.76
, 2 & 0.95 respectively.
Reference
[1.] M.S.Soylemez, M.Unsal(1997) Optimum
Insulation Thickness for Refrigerant
applications, Energy Conservation and
Management 40(1999) 13-21.
[2.] ASHRAE Handbook of Fundamentals,
1993.
[3.] B.Kundu- international communications in
heat and mass transfer,2002.(An analytica
study of the effect of dehumidification of air
on the performance and optimization of
straight tapered fins.
[4.] Process heat transfer by DONAL Q. KERN
(MCGRAW-HILL).
[5.] Mathematics department of Massachusettes
institute of technology.

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Theoretical Convective Heat Transfer Model Developement of Cold Storage Using Taguchi Analysis.

  • 1. Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17 www.ijera.com 13 | P a g e Theoretical Convective Heat Transfer Model Developement of Cold Storage Using Taguchi Analysis. Dr.N.Mukhopadhyay1 , Suman Debnath2 , 1 Assistant Professor, Department of Mechanical Engineering, Jalpaiguri Government Engineering College 2 Post Graduate Scholar, Department of Mechanical Engineering,Jalpaiguri Government Engineering College, India. Abstract Energy crisis is one of the most important problems the world is facing now-a-days. With the increase of cost of electrical energy operating cost of cold storage storing is increasing which forces the increased cost price of the commodities that are kept. In this situation if the maximum heat energy(Q) is absorbed by the evaporator inside the cold room through convective heat transfer process in terms of –heat transfer due to convection and heat transfer due to condensation, more energy has to be wasted to maintain the evaporator space at the desired temperature range of 2- 8 degree centigrade. In this paper we have proposed a theoretical heat transfermodel of convective heat transfer incold storage using Taguchi L9 orthogonal array. Velocity of air(V), Temperature difference(dT), RelativeHumidity(RH)are the basic variable and three ranges are taken each of them in the model development. Graphical interpretations from the model justifies the reality Keywords: cold storage, convective heat transfer model, heat absorbed by evaporator, Taguchi Analysis. I. Introduction Demand for cold storages have been increasing rapidly over the past couple of decades so that food commodities can be uniformly supplied all through the year and food items are prevented from perishing. India is having a unique geographical position and a wide range of soil thus producing variety of fruits and vegetables like apples, grapes, oranges, potatoes, chilies, ginger, etc. Marine products are also being produced in large quantities due to large coastal areas. The cold storage facilities are the prime infrastructural component for such perishable commodities. Besides the role of stabilizing market prices and evenly distributing both on demand basis and time basis, the cold storage industry provide other advantages and benefits to both the farmers and the consumers. The farmers get the opportunity to get a good return of their hard work. On the consumer sides they get the perishable commodities with lower fluctuation of price. Very little theoretical and experimental studies are being reported in the journal on the performance enhancement of cold storage. Energy crisis is one of the most important problems the world is facing nowadays. With the increase of cost of electrical energy operating cost of cold storage storing is increasing which forces the increased cost price of the commodities that are kept. So it is very important to make cold storage energy efficient or in the other words reduce its energy consumption. Thus the storage cost will eventually comes down. In case of conduction we have to minimize the leakage of heat through wall but in convection maximum heat should be absorbed by refrigerant to create cooling uniformity thought out the evaporator space.If the desirable heat is not absorbed by tube or pipe refrigerant then temp of the refrigerated space will be increased, which not only hamper the quality of the product which has been stored there but reduces the overall performance of the plant. That’s why a mathematical modeling is absolutely necessary to predict the performance. In this paper we have proposed a theoretical heat transfer model of convective heat transfer model development of a cold storage using Taguchi L9 orthogonal array. Velocity of air (V), Temperature difference (dT), Relative Humidity (RH)are the basic variables and three ranges are taken each of them in the model development. Graphical interpretations from the model justifies the reality II. Model development Relationship between heat gain & energy consumption is given by E= (Q t)/COP [M.S.Soylemez, M.Unsal ](1997) [1] E=energy consumption of refrigeration system (kw/h), t=equivalent full load hours of operation of refrigeration system(hrs), COP= co efficient of performance of refrigeration plant., Q= heat energy extracted from cold room (Joule) Response variableis heat transfer due to convection and condensation and predictor variables are Velocity of air (V), Temperature difference (dT), Relative Humidity (RH) .With the help of Taguchi methodology we construct our design matrix. RESEARCH ARTICLE OPEN ACCESS
  • 2. Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17 www.ijera.com 14 | P a g e Orthogonal arrays provide a best set of well balanced (minimum) experiments .It was developed by C.R.Rao (1947) Popularized by Gene chi Taguchi (1987).The number of rows of an orthogonal array represents the requisite number of experiments. III. Regression analysis Regression analysis is the relationship between various variables. By regression analysis one can construct a relationship between response variable and predictor variable. It demonstrates what will be the changes in response variable because of the changes in predictor variable. Simple regression equation is y=a+ b x In this problem more than one predictor variable is involved and hence simple regression analysis can not be used. We have to take the help of multiple regression analysis. There are two types of multiple regression analysis- 1) Simple multiple regression analysis (regression equation of first order) 2) Polynomial multiple regression analysis (regression equation of second order or more) Simple multiple regression analysis is represented by the equation of first order regression Y= β0+β1X1+β2X2+β3X3+…………………..+ε Where β is constant terms & X is the variables & ε is the experimental error. Polynomial multiple regression analysis equation is Y = β0+ β1X1+β2X2+β3X3+ β 11X2 11+ β 22X2 22+ β33X2 33+ β12X1X2+ β13X1X3+ β23X2X3 The above equation is second order polynomial equation for 3 variables. Where β are constant, X1 , X2 , X3 are the linear terms, X12 X13 X23 are the interaction terms between the factors, and lastly X11 X22 X33 are the square terms. Q (heat due to conv+condensation) = response variable, V, dT, RH= predictor variable. Polynomial regression equation becomes after replacing real problem variables Q (heat due to conv+condensation) = β0+β1(V)+β2 (dT)+β3 (RH)+ β 11 (V)*(V)+ β 22(dT)*(dT)+β33 (RH)*(RH)+ β12(V)*(dT)+ β13(dT)*(RH)+ β23(RH)*(V) To solve this equation following matrix method is used Y= [β][ X ] [β]=Y [X-1 ] where [β] is the coefficient matrix, Y is the response variable matrix; [X-1] is the inverse of predictor variable matrix. In this problem there are 3 independent variables and each variable has 3 levels and hence from the Taguchi Orthogonal Array (OA) table L9 OA is best selected. Cold storage Description The overall dimensions of cold storage plant are 87.5mx34.15mx16.77m.The cold storage building is of five floors with each floor having 2 cold chambers of 43.25m x 17m sizes operating at different temperature as per the requirements of commodities. For our analysis purpose we only considered zone 1 which is referred as cold room. IV. Parameter &Range Selection The one chamber of cold storage Length ,Breath and Height 87.5m,34.15m and 16.77m respectively. The three values of air velocity(V) of evaporator space are 0.74m/s, 1.25m/s and 1.76m/s respectively. The three values of temperature difference (dT) of evaporator space are 2, 5 & 8 centigrade respectively. The three values of relative humidity (RH) of evaporative space are 0.85, 0.90 & 0.95 respectively. V. Heat (heat due to conv+condensation) Calculation In this study heat transfer from evaporating space to refrigerant (which are in tube or pipe) only being considered. The transfer heat evaporating space to refrigerant are calculated in terms of velocity of air (V), temp. difference (dT) & relative humidity RH) . Only convection heat transfer effect is being considered in this study. Basic equation for heat transfer QT = Qconv+ Qcondensation. Qconv=AhcdT&Qcondensation=Ahm(RH)hfg. Here Qconv=heat transfer due to convection &Qcondensation=heat transfer due to condensation & QT=Total heat transfer or absorb heat into refrigerant . And hc/hm=cp(Le)2/3 &hcL/K=Nu=0.026(Re)0.8 (Pr)0.3 The final heat transfer equation due to velocity of air (V), temp. difference (dT) & relative humidity RH) is QT=7.905V0.8 (dT + 2490 RH). Hera A=surface area of tubes in evaporator space 1872 m2 .hc=convective heat transfer co-efficient. hm=convective mass transfer co-efficient.hfg=latent heat of condensation of moisture 2490 KJ/Kg-K. Cp=specific heat of air 1.005 KJ/Kg-K. Le=Lewis number for air it is one. After getting the full observation table which include all the predictor variables and response variable, values can be computed easily in the following equation- Q (heat due to conv+condensation) = β0+β1(V)+β2 (dT)+β3 (RH)+ β 11 (V)*(V)+ β 22(dT)*(dT)+β33 (RH)*(RH)+ β12(V)*(dT)+ β13(dT)*(RH)+ β23(RH)*(V) We get nineequations but number of unknowns are ten. Now we can solvethese equations-eliminate some of variables in terms of others. Then we get[ X ] matrix as [9*9]. We also get response variable matrix [Q] which is a [9*1] matrix. With the help of following equation we can get the co efficient values- [β]=[Q]*[X-1 ] where [x]-denotes the variable matrix. The proposed theoretical mathematical model for heat transfer in cold storage is –
  • 3. Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17 www.ijera.com 15 | P a g e Q (heat due to conv+condensation) = -770+2791(V)- 34(dT)+2791(RH)-1143(V)*(V)- 1(dT)*(dT)+772(RH)*(RH)+ 9(V)*(dT)+ 46(dT)*(RH)+ 15230(RH)*(V) . VI. Results and Discussions L9 OA combination Table with notation for Matrix design- L9 table with various factors level TABLE 1 TABLE 2 Levels Velocity of air (V)(m/s) Temperature difference(dT)(c entrigade) Relative humidity 1 0.74 2 0.85 2 1.25 5 0.90 3 1.76 8 0.95 Observation table TABLE 3 Obs no - V dT RH Q 1 0.74 2 0.85 13162.61 2 0.74 5 0.90 13954.63 3 0.74 8 0.95 14746.05 4 1.25 2 0.90 21196.58 5 1.25 5 0.95 22401.23 6 1.25 8 0.85 20075.48 7 1.76 2 0.95 29416.29 8 1.76 5 0.85 26359.37 9 1.76 8 0.90 27944.56 V dT RH 0.74 2 0.85 0.74 5 0.90 0.74 8 0.95 1.25 2 0.90 1.25 5 0.95 1.25 8 0.85 1.76 2 0.95 1.76 5 0.85 1.76 8 0.90
  • 4. Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17 www.ijera.com 16 | P a g e Figure 1: variation of heat transfer with air velocity. Figure 1 shows that heat absorption increase with velocity of air increases . Figure 2 : variation of heat transfer with temperature difference. Figure 2 shows that heat absorption increase with temperature difference increase and at lower temperature difference it is more effected than the higher temperature difference.
  • 5. Dr. N. Mukhopadhyay Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 5, Issue 1, ( Part -6) January 2015, pp.13-17 www.ijera.com 17 | P a g e Figure 3 : variation of heat transfer with relative humidity. Figure 3 shows that heatabsorption increase with increase in relative humidity but in this case gradient is higher than the figure 2 case. VII. Conclusion 1.with increasing the velocity of air ,temperature difference and relative humidity heat absorb by the refrigerant is increased. 2.To create maximum cooling effects maximum heat transfer is required at the values of air velocity, temperature difference and relative humidity are 1.76 , 2 & 0.95 respectively. Reference [1.] M.S.Soylemez, M.Unsal(1997) Optimum Insulation Thickness for Refrigerant applications, Energy Conservation and Management 40(1999) 13-21. [2.] ASHRAE Handbook of Fundamentals, 1993. [3.] B.Kundu- international communications in heat and mass transfer,2002.(An analytica study of the effect of dehumidification of air on the performance and optimization of straight tapered fins. [4.] Process heat transfer by DONAL Q. KERN (MCGRAW-HILL). [5.] Mathematics department of Massachusettes institute of technology.