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Optimization ofAir Preheater for compactness of shell by
evaluating performance for different Baffle structure
Nemish Kanwar1* and Dr P Srinivasan2*
1
BE(Hons) Mechanical Engineering, 2
Associate Professor
*Department of Mechanical Engineering, Birla Institute of Technology and Science, Pilani,
Rajasthan 333031, India
1
Corressponding author, email: nemishkanwar@gmail.com
ABSTRACT:
Designing of an Air Preheater with increased performance from an existing design
through alteration in baffle placement. Analysis of 4 Baffle designs for segmented Baffle
case was done using Ansys Fluent. The net heat recovery rate was computed by
subtracting pump work from heat recovered. Based on the result, Air Preheater design
was recommended.
Keywords: Heat Transfer, Numerical Analysis, Simulation, Baffle Arrangement
1. INTRODUCTION
Air Preheater is designed to heat air before another processes. The purpose of Air Preheater is
to recover heat from boiler flue gas which increases thermal efficiency of boiler by reducing
useful heat lost in flue gas 1
. As a result, Flue gas temperature is reduced in the stack. It also
allows temperature control over temperature of gases leaving stack. Air Preheaters are
generally divided into 2 types: Regenerative and Recuperative. Regenerative type has an
energy storage matrix which is alternatively exposed to hot and cold fluids. In Recuperative
type, heat is transferred between hot gases to air across heat exchanging surface2
. They are
plate type and tubular, although tubular type is generally used. Tubular units are essentially
counter-flow shell and tube in which hot gases flow inside the tubes and the air flows outside
in the shell. Baffles are provided to maximize air contact with tubes.
Shell and tube heat exchangers are probably the most widespread and commonly used
equipment in the process industries. They are essential equipment for all the major industries
like chemical and petrochemical plants, oil refineries, power plants and metallurgical
operations. They are employed for several applications such as heating, cooling, condensation
and boiling. There are several reasons for their general acceptance. Firstly, these equipment
provide a comparatively large ratio of heat transfer area to volume as well as weight. It is
relatively easy to construct in a wide range of sizes and which is mechanically rugged enough
to withstand the normal shop fabrication stresses, shipping and field erection stresses, and
normal operating conditions. There are many versions of the basic configuration, which can be
used to solve special problems. The shell and tube exchanger can be cleaned reasonably easily.
Further, the components which are most subject to failure, gaskets and tubes, can be easily
replaced. Finally, fairly good design methods and standards exist, and the expertise and shop
2
facilities for the successful design and construction of shell and tube exchangers are universally
available 3
.
The basic principle of a shell and tube heat exchanger is that two fluids flow at different
temperatures separated by a wall. Owing to the temperature difference, heat transfer from fluid
at higher temperature to lower temperature occurs by mechanism of conduction and
convection. The shell side flow in a shell and tube heat exchanger is quite complicated. The
inlet and outlet being perpendicular to general flow direction brings complexities in shell flow.
In addition, the presence of baffles makes the flow further complex. It is thus desirable to
understand the flow field and hence, in turn, be able to predict the heat transfer mechanism
over a wide range of heat duty and mass velocities on both the sides.
During the past 25 years, (CFD) computational fluid dynamics is being increasingly used
because of the developments in the computational power as well as numerical techniques. It is
being used as a quick and efficient tool to assess the flow distribution and heat transfer in
various types of heat exchangers. 4
investigated the overall heat transfer rate and the pressure
drop through shell side with helical baffles by using commercial CFD code FLUENT and the
authors obtained good agreement between the CFD predictions and the experimental
measurements.
5
also used FLUENT 6.3 for the CFD simulations. The simulations were performed using
standard k–Ρ,2nd order k–Ρ, realizable k–Ρ model and Spallart–Allmaras turbulence models.
The number of baffles was varied from 6 to 12. Heat transfer was evaluated by log mean
temperature difference (LMTD) from the temperature profiles obtained from the simulations.
The studies were focused on the effects of various types of baffle and their cut, spacing, etc. on
the pressure drop and heat transfer.
Figure 1: Effect of baffle cut and baffle spacing on the shell side main stream: (a) small baffle cut, (b)
large baffle cut, (c) small baffle spacing, (d) large baffle spacing, (e) ideal 5
This report focuses on cuboidal shell design for a shell and tube Air Preheater. Air flows in
the shell and Flue gas flows inside the tube in counter flow.
3
The geometry is a 970π‘šπ‘š Γ— 650π‘šπ‘š Γ— 4200π‘šπ‘š cuboidal shell with 12 Γ— 8 quantity of tubes
with external diameter 64π‘šπ‘š and thickness 1.63 π‘šπ‘š. Mass flow rate of air and gas supplied
are 3.07 π‘˜π‘”/𝑠 and 3.24π‘˜π‘”/𝑠 with inlet temperatures 27°𝐢 and 360°𝐢 respectively.
The main aim of this report is to illustrate change in heat recovery rate and pressure changes
for different baffle arrangements. Baffle spacing between 4 baffles in an arrangement is kept
constant. The transverse view of APH is divided into 4 quadrants and named 1,2,3,4
respectively.
The order of baffle position in the direction of air flow is used to name a baffle arrangement.
A total of 4 baffle arrangements have been chosen keeping all the other parameters fixed- 1-3-
1-3, 1-2-3-4, 12-34-12-34 and 0-0-0-0. semi baffle and no baffle names are used instead of 12-
34-12-34 and 0-0-0-0 respectively throughout this document for simplification.
2. CFD MODELLING
1.1 PHYSICAL MODELLING
The geometry was drawn and meshed by using GAMBIT 2.2.30. Original Air Preheater is
compared with 3 different segmented Air Preheaters with alternative Baffle designs.
The original APH had rectangular baffles in 1-3-1-3 format. The three other designs are: No
baffle, 1-2-3-4 format and semi-baffles.
Governing equations and boundary conditions The commercial CFD code Fluent 6.3 was used
to perform the simulation. Since the Re number of fluid in this article was in the range from
dozens to hundreds of thousands, the simulations were solved employing the laminar flow
model and the renormalization group (Standard) kβ€“πœ– model. Choosing (Standard) kβ€“πœ– model
as the turbulence model was because it involved the effect of swirl on turbulence, which could
enhance the simulation accuracy of swirling existed in the heat exchanger; plus, the (Standard)
kβ€“πœ– model had already gained excellent utilization in some published articles about heat
exchanger simulation. The governing equations for continuity, momentum, energy, k and πœ–
were used in the computation.
Table 1: Thermo physical properties of Air (polynomial equation)
Property π‘₯0
π‘₯βˆ’1
π‘₯βˆ’2
Density (kg/m3) 2.35 -0.0051 3.57E-06
Cp (J/kg K) 1014 -0.1153 0.000296
Thermal Conductivity
(W/m K)
0.002753 8.58E-
05
-2.28E-
08
Dynamic Viscosity
(kg/Pa s)
2.95E-06 5.79E-
08
-1.91E-
11
4
Table 2: Thermo physical properties of Flue Gas (polynomial equation)
Property π‘₯0
π‘₯βˆ’1
π‘₯βˆ’2
π‘₯βˆ’3
π‘₯βˆ’4
π‘₯βˆ’5
π‘₯βˆ’6
π‘₯βˆ’7
Density
(kg/m3)
3.892 -0.017 3.98E-
05
-
5.38E
-08
4.36E
-11
-
2.10E
-14
5.41E
-18
-
5.90E
-22
Cp (J/kg K) 965.9 0.646 -
0.00398
1.16E
-05
-
1.66E
-08
1.29E
-11
-
5.34E
-15
9.17E
-19
Thermal
Conductivity
(W/m K)
0.00017
4
0.00010
4
-7.01E-
08
4.38E
-11
-
1.17E
-14
- - -
Dynamic
Viscosity
(kg/Pa s)
6.62E-
07
7.41E-
08
-5.77E-
11
3.60E
-14
-
9.59E
-18
- - -
1.2 MESH SELECTION
Mesh generation for segmented baffle design was performed using Gambit. The whole
volume was meshed using Hex/Wedge Cooper scheme with mesh size 10. Mesh was
successfully generated error-free.
1.3 NUMERICAL METHOD
The governing equations along with the boundary conditions were iteratively solved by the
finite volume method using SIMPLE pressure–velocity coupling algorithm. The QUICK
scheme with first-order precision was utilized for convective formulation and the SIMPLE
algorithm was for pressure-velocity coupling
The convergence criteria were 10βˆ’3
for energy, x-y-z velocities and 10βˆ’2
for Turbulent Kinetic
Energy, π‘˜ and 10βˆ’1
for turbulent dissipation, πœ–. The calculation was carried out in Dell
Workstation in IPC, BITS Pilani with 8GB RAM and 3.1 GHz CPU.
Air and flue gas property was taken as polynomial equation with coefficients in Table 1 and
Table 2 respectively.
3. RESULTS
The 4 segmented Baffle case were simulated in Fluent. It is crucial to determine flue gas outlet
temperature profile (see Figure 2) Pressure drop and average temperature at outlet should be
least for the best case. In this case, Temperature profile of A shows many regions with
temperature 310Β°C.
The flue gas domain is above sulphur dew point temperature (170°𝐢) which marks it safe from
sulphur corrosion.
.
5
Figure 2: Flue Gas Outlet temperature of A. 1-3-1-3 baffle geometry, B. 1-2-3-4 baffle geometry, C.
Semi Baffle geometry, D. No Baffle geometry
Figure 3 illustrates the streamlines in the air domain, where dark blue lines shows dead zone
formation where flow is stagnant. Heat transfer coefficient is least in these zone because of low
Reynolds number. 2 out of 4 quarters mostly comprise of dead zones in 1-3-1-3 arrangement;
resulting in very low heat transfer from these tube bundles.
Figure 3: Streamlines Air Domain of A. 1-3-1-3 baffle geometry, B. 1-2-3-4 baffle geometry, C. Semi
Baffle geometry, D. No Baffle geometry (air flow is from left to right)
6
Table 3: Summary of average temperature at all the inlets and outlets
1-2-3-4 1-3-1-3 no Baffle Semi
Baffles
Airin °𝐢 26.85 26.85 26.85 26.85
airout1 °𝐢 133.59 126.92 131.08 135.29
airout2 °𝐢 149.88 150.45 160.29 187.04
Fluein °𝐢 340.07 339.01 343.97 339.50
Flueout °𝐢 234.38 238.27 235.78 229.73
The overall heat transfer coefficient and effectiveness needs to be computed for each case for
comparison.
Heat transfer coefficient can be calculated using LMTD approach
π‘ˆπ΄(𝐿𝑀𝑇𝐷) = π‘šπ‘ 𝑝Δ𝑇
Effectiveness of a Heat exchanger is used to evaluate performance.
πœ– =
𝐢𝑓𝑙𝑒𝑒(𝑇𝑓𝑙𝑒𝑒 𝑖𝑛
βˆ’ 𝑇𝑓𝑙𝑒𝑒 π‘œπ‘’π‘‘
)
𝐢 π‘šπ‘–π‘›(𝑇𝑓𝑙𝑒𝑒 𝑖𝑛
βˆ’ π‘‡π‘Žπ‘–π‘Ÿ π‘œπ‘’π‘‘
)
Table 4 shows the heat recovery rate from the exiting flue gas and fan work required for air
and gas circulation. Assuming, 40% efficiency of thermal plant and 75% FD fan efficiency and
90% motor efficiency, Net heat recovered is calculated. Heat recovered is maximum for No
Baffle structure, followed by 1-2-3-4, 1-3-1-3, Semi Baffles.
Table 4: Net Heat Recovered from different designs
1-2-3-4 1-3-1-3
No
Baffle
Semi
Baffles
Fan work
Total, W
3247 3576 2562 12036
Heat
recovered,
W
358116 341450 366787 371748
Net heat
recovered
138436 131282 142919 130868
7
Table 5: Performance Parameters of Air preheaters and Pressure drops in flow stream
1-2-3-4 1-3-1-3 no Baffle Semi Baffles
U, 𝐖/𝐦 𝟐
𝐊 21.09 19.86 20.90 23.21
Effectiveness 36.86% 35.27% 37.28% 38.32%
Pressure drop_air 𝑷𝒂 841.190198 841.2309693 576.4366207 2391.179035
Pressure drop_flue 𝑷𝒂 116.82776 118.55953 118.06029 115.98264
4. CONCLUSIONS
Formation of large amounts of wake region (see Figure 3) in 1-3-1-3 arrangement explains the
temperature profile, in Figure 2, which shows several regions with 310°𝐢 temperature.
The overall heat transfer coefficient and effectiveness for different baffle arrangements are
determined via numerical analysis using a method based on convective mass transfer. Results shown
in
Table 5, dictates that arrangements 1-2-3-4 and semi baffle gives better results than commercial
Air preheater model with 1-3-1-3 arrangement. Pressure drop is same for 1-2-3-4, while it is
increased for semi baffle case.
Referring Table 4, Air preheater without baffles is the clear choice; but it is not used for
vibrational stability of tubes. So, the next better 1-2-3-4 arrangement should be used instead of
conventional 1-3-1-3 arrangement as it has more heat recovery rate.
5. REFERENCES
1. Kakac, S. & Liu, H. Heat Exchangers Selection, Rating and Thermal Design. (CRC
PRESS, 2002).
2. Nag, P. K. Power Plant Engineering. (Tata McGraw-Hill Publishing Company Limited,
2008).
3. Pal, E., Kumar, I., Joshi, J. B. & Maheshwari, N. K. CFD simulations of shell-side flow
in a shell-and-tube type heat exchanger with and without baffles. Chem. Eng. Sci. 143,
314–340 (2016).
4. Wang, Q., Chen, Q., Chen, G. & Zeng, M. Numerical investigation on combined
multiple shell-pass shell-and-tube heat exchanger with continuous helical baffles. Int. J.
Heat Mass Transf. 52, 1214–1222 (2009).
5. Ozden, E. & Tari, I. Shell side CFD analysis of a small shell-and-tube heat exchanger.
Energy Convers. Manag. 51, 1004–1014 (2010).

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  • 1. 1 Optimization ofAir Preheater for compactness of shell by evaluating performance for different Baffle structure Nemish Kanwar1* and Dr P Srinivasan2* 1 BE(Hons) Mechanical Engineering, 2 Associate Professor *Department of Mechanical Engineering, Birla Institute of Technology and Science, Pilani, Rajasthan 333031, India 1 Corressponding author, email: nemishkanwar@gmail.com ABSTRACT: Designing of an Air Preheater with increased performance from an existing design through alteration in baffle placement. Analysis of 4 Baffle designs for segmented Baffle case was done using Ansys Fluent. The net heat recovery rate was computed by subtracting pump work from heat recovered. Based on the result, Air Preheater design was recommended. Keywords: Heat Transfer, Numerical Analysis, Simulation, Baffle Arrangement 1. INTRODUCTION Air Preheater is designed to heat air before another processes. The purpose of Air Preheater is to recover heat from boiler flue gas which increases thermal efficiency of boiler by reducing useful heat lost in flue gas 1 . As a result, Flue gas temperature is reduced in the stack. It also allows temperature control over temperature of gases leaving stack. Air Preheaters are generally divided into 2 types: Regenerative and Recuperative. Regenerative type has an energy storage matrix which is alternatively exposed to hot and cold fluids. In Recuperative type, heat is transferred between hot gases to air across heat exchanging surface2 . They are plate type and tubular, although tubular type is generally used. Tubular units are essentially counter-flow shell and tube in which hot gases flow inside the tubes and the air flows outside in the shell. Baffles are provided to maximize air contact with tubes. Shell and tube heat exchangers are probably the most widespread and commonly used equipment in the process industries. They are essential equipment for all the major industries like chemical and petrochemical plants, oil refineries, power plants and metallurgical operations. They are employed for several applications such as heating, cooling, condensation and boiling. There are several reasons for their general acceptance. Firstly, these equipment provide a comparatively large ratio of heat transfer area to volume as well as weight. It is relatively easy to construct in a wide range of sizes and which is mechanically rugged enough to withstand the normal shop fabrication stresses, shipping and field erection stresses, and normal operating conditions. There are many versions of the basic configuration, which can be used to solve special problems. The shell and tube exchanger can be cleaned reasonably easily. Further, the components which are most subject to failure, gaskets and tubes, can be easily replaced. Finally, fairly good design methods and standards exist, and the expertise and shop
  • 2. 2 facilities for the successful design and construction of shell and tube exchangers are universally available 3 . The basic principle of a shell and tube heat exchanger is that two fluids flow at different temperatures separated by a wall. Owing to the temperature difference, heat transfer from fluid at higher temperature to lower temperature occurs by mechanism of conduction and convection. The shell side flow in a shell and tube heat exchanger is quite complicated. The inlet and outlet being perpendicular to general flow direction brings complexities in shell flow. In addition, the presence of baffles makes the flow further complex. It is thus desirable to understand the flow field and hence, in turn, be able to predict the heat transfer mechanism over a wide range of heat duty and mass velocities on both the sides. During the past 25 years, (CFD) computational fluid dynamics is being increasingly used because of the developments in the computational power as well as numerical techniques. It is being used as a quick and efficient tool to assess the flow distribution and heat transfer in various types of heat exchangers. 4 investigated the overall heat transfer rate and the pressure drop through shell side with helical baffles by using commercial CFD code FLUENT and the authors obtained good agreement between the CFD predictions and the experimental measurements. 5 also used FLUENT 6.3 for the CFD simulations. The simulations were performed using standard k–Ρ,2nd order k–Ρ, realizable k–Ρ model and Spallart–Allmaras turbulence models. The number of baffles was varied from 6 to 12. Heat transfer was evaluated by log mean temperature difference (LMTD) from the temperature profiles obtained from the simulations. The studies were focused on the effects of various types of baffle and their cut, spacing, etc. on the pressure drop and heat transfer. Figure 1: Effect of baffle cut and baffle spacing on the shell side main stream: (a) small baffle cut, (b) large baffle cut, (c) small baffle spacing, (d) large baffle spacing, (e) ideal 5 This report focuses on cuboidal shell design for a shell and tube Air Preheater. Air flows in the shell and Flue gas flows inside the tube in counter flow.
  • 3. 3 The geometry is a 970π‘šπ‘š Γ— 650π‘šπ‘š Γ— 4200π‘šπ‘š cuboidal shell with 12 Γ— 8 quantity of tubes with external diameter 64π‘šπ‘š and thickness 1.63 π‘šπ‘š. Mass flow rate of air and gas supplied are 3.07 π‘˜π‘”/𝑠 and 3.24π‘˜π‘”/𝑠 with inlet temperatures 27°𝐢 and 360°𝐢 respectively. The main aim of this report is to illustrate change in heat recovery rate and pressure changes for different baffle arrangements. Baffle spacing between 4 baffles in an arrangement is kept constant. The transverse view of APH is divided into 4 quadrants and named 1,2,3,4 respectively. The order of baffle position in the direction of air flow is used to name a baffle arrangement. A total of 4 baffle arrangements have been chosen keeping all the other parameters fixed- 1-3- 1-3, 1-2-3-4, 12-34-12-34 and 0-0-0-0. semi baffle and no baffle names are used instead of 12- 34-12-34 and 0-0-0-0 respectively throughout this document for simplification. 2. CFD MODELLING 1.1 PHYSICAL MODELLING The geometry was drawn and meshed by using GAMBIT 2.2.30. Original Air Preheater is compared with 3 different segmented Air Preheaters with alternative Baffle designs. The original APH had rectangular baffles in 1-3-1-3 format. The three other designs are: No baffle, 1-2-3-4 format and semi-baffles. Governing equations and boundary conditions The commercial CFD code Fluent 6.3 was used to perform the simulation. Since the Re number of fluid in this article was in the range from dozens to hundreds of thousands, the simulations were solved employing the laminar flow model and the renormalization group (Standard) kβ€“πœ– model. Choosing (Standard) kβ€“πœ– model as the turbulence model was because it involved the effect of swirl on turbulence, which could enhance the simulation accuracy of swirling existed in the heat exchanger; plus, the (Standard) kβ€“πœ– model had already gained excellent utilization in some published articles about heat exchanger simulation. The governing equations for continuity, momentum, energy, k and πœ– were used in the computation. Table 1: Thermo physical properties of Air (polynomial equation) Property π‘₯0 π‘₯βˆ’1 π‘₯βˆ’2 Density (kg/m3) 2.35 -0.0051 3.57E-06 Cp (J/kg K) 1014 -0.1153 0.000296 Thermal Conductivity (W/m K) 0.002753 8.58E- 05 -2.28E- 08 Dynamic Viscosity (kg/Pa s) 2.95E-06 5.79E- 08 -1.91E- 11
  • 4. 4 Table 2: Thermo physical properties of Flue Gas (polynomial equation) Property π‘₯0 π‘₯βˆ’1 π‘₯βˆ’2 π‘₯βˆ’3 π‘₯βˆ’4 π‘₯βˆ’5 π‘₯βˆ’6 π‘₯βˆ’7 Density (kg/m3) 3.892 -0.017 3.98E- 05 - 5.38E -08 4.36E -11 - 2.10E -14 5.41E -18 - 5.90E -22 Cp (J/kg K) 965.9 0.646 - 0.00398 1.16E -05 - 1.66E -08 1.29E -11 - 5.34E -15 9.17E -19 Thermal Conductivity (W/m K) 0.00017 4 0.00010 4 -7.01E- 08 4.38E -11 - 1.17E -14 - - - Dynamic Viscosity (kg/Pa s) 6.62E- 07 7.41E- 08 -5.77E- 11 3.60E -14 - 9.59E -18 - - - 1.2 MESH SELECTION Mesh generation for segmented baffle design was performed using Gambit. The whole volume was meshed using Hex/Wedge Cooper scheme with mesh size 10. Mesh was successfully generated error-free. 1.3 NUMERICAL METHOD The governing equations along with the boundary conditions were iteratively solved by the finite volume method using SIMPLE pressure–velocity coupling algorithm. The QUICK scheme with first-order precision was utilized for convective formulation and the SIMPLE algorithm was for pressure-velocity coupling The convergence criteria were 10βˆ’3 for energy, x-y-z velocities and 10βˆ’2 for Turbulent Kinetic Energy, π‘˜ and 10βˆ’1 for turbulent dissipation, πœ–. The calculation was carried out in Dell Workstation in IPC, BITS Pilani with 8GB RAM and 3.1 GHz CPU. Air and flue gas property was taken as polynomial equation with coefficients in Table 1 and Table 2 respectively. 3. RESULTS The 4 segmented Baffle case were simulated in Fluent. It is crucial to determine flue gas outlet temperature profile (see Figure 2) Pressure drop and average temperature at outlet should be least for the best case. In this case, Temperature profile of A shows many regions with temperature 310Β°C. The flue gas domain is above sulphur dew point temperature (170°𝐢) which marks it safe from sulphur corrosion. .
  • 5. 5 Figure 2: Flue Gas Outlet temperature of A. 1-3-1-3 baffle geometry, B. 1-2-3-4 baffle geometry, C. Semi Baffle geometry, D. No Baffle geometry Figure 3 illustrates the streamlines in the air domain, where dark blue lines shows dead zone formation where flow is stagnant. Heat transfer coefficient is least in these zone because of low Reynolds number. 2 out of 4 quarters mostly comprise of dead zones in 1-3-1-3 arrangement; resulting in very low heat transfer from these tube bundles. Figure 3: Streamlines Air Domain of A. 1-3-1-3 baffle geometry, B. 1-2-3-4 baffle geometry, C. Semi Baffle geometry, D. No Baffle geometry (air flow is from left to right)
  • 6. 6 Table 3: Summary of average temperature at all the inlets and outlets 1-2-3-4 1-3-1-3 no Baffle Semi Baffles Airin °𝐢 26.85 26.85 26.85 26.85 airout1 °𝐢 133.59 126.92 131.08 135.29 airout2 °𝐢 149.88 150.45 160.29 187.04 Fluein °𝐢 340.07 339.01 343.97 339.50 Flueout °𝐢 234.38 238.27 235.78 229.73 The overall heat transfer coefficient and effectiveness needs to be computed for each case for comparison. Heat transfer coefficient can be calculated using LMTD approach π‘ˆπ΄(𝐿𝑀𝑇𝐷) = π‘šπ‘ 𝑝Δ𝑇 Effectiveness of a Heat exchanger is used to evaluate performance. πœ– = 𝐢𝑓𝑙𝑒𝑒(𝑇𝑓𝑙𝑒𝑒 𝑖𝑛 βˆ’ 𝑇𝑓𝑙𝑒𝑒 π‘œπ‘’π‘‘ ) 𝐢 π‘šπ‘–π‘›(𝑇𝑓𝑙𝑒𝑒 𝑖𝑛 βˆ’ π‘‡π‘Žπ‘–π‘Ÿ π‘œπ‘’π‘‘ ) Table 4 shows the heat recovery rate from the exiting flue gas and fan work required for air and gas circulation. Assuming, 40% efficiency of thermal plant and 75% FD fan efficiency and 90% motor efficiency, Net heat recovered is calculated. Heat recovered is maximum for No Baffle structure, followed by 1-2-3-4, 1-3-1-3, Semi Baffles. Table 4: Net Heat Recovered from different designs 1-2-3-4 1-3-1-3 No Baffle Semi Baffles Fan work Total, W 3247 3576 2562 12036 Heat recovered, W 358116 341450 366787 371748 Net heat recovered 138436 131282 142919 130868
  • 7. 7 Table 5: Performance Parameters of Air preheaters and Pressure drops in flow stream 1-2-3-4 1-3-1-3 no Baffle Semi Baffles U, 𝐖/𝐦 𝟐 𝐊 21.09 19.86 20.90 23.21 Effectiveness 36.86% 35.27% 37.28% 38.32% Pressure drop_air 𝑷𝒂 841.190198 841.2309693 576.4366207 2391.179035 Pressure drop_flue 𝑷𝒂 116.82776 118.55953 118.06029 115.98264 4. CONCLUSIONS Formation of large amounts of wake region (see Figure 3) in 1-3-1-3 arrangement explains the temperature profile, in Figure 2, which shows several regions with 310°𝐢 temperature. The overall heat transfer coefficient and effectiveness for different baffle arrangements are determined via numerical analysis using a method based on convective mass transfer. Results shown in Table 5, dictates that arrangements 1-2-3-4 and semi baffle gives better results than commercial Air preheater model with 1-3-1-3 arrangement. Pressure drop is same for 1-2-3-4, while it is increased for semi baffle case. Referring Table 4, Air preheater without baffles is the clear choice; but it is not used for vibrational stability of tubes. So, the next better 1-2-3-4 arrangement should be used instead of conventional 1-3-1-3 arrangement as it has more heat recovery rate. 5. REFERENCES 1. Kakac, S. & Liu, H. Heat Exchangers Selection, Rating and Thermal Design. (CRC PRESS, 2002). 2. Nag, P. K. Power Plant Engineering. (Tata McGraw-Hill Publishing Company Limited, 2008). 3. Pal, E., Kumar, I., Joshi, J. B. & Maheshwari, N. K. CFD simulations of shell-side flow in a shell-and-tube type heat exchanger with and without baffles. Chem. Eng. Sci. 143, 314–340 (2016). 4. Wang, Q., Chen, Q., Chen, G. & Zeng, M. Numerical investigation on combined multiple shell-pass shell-and-tube heat exchanger with continuous helical baffles. Int. J. Heat Mass Transf. 52, 1214–1222 (2009). 5. Ozden, E. & Tari, I. Shell side CFD analysis of a small shell-and-tube heat exchanger. Energy Convers. Manag. 51, 1004–1014 (2010).