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INTERNATIONAL JOURNAL OF ADVANCED RESEARCH 
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 
6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 
IN ENGINEERING AND TECHNOLOGY (IJARET) 
ISSN 0976 - 6480 (Print) 
ISSN 0976 - 6499 (Online) 
Volume 5, Issue 7, July (2014), pp. 39-46 
© IAEME: http://www.iaeme.com/IJARET.asp 
Journal Impact Factor (2014): 7.8273 (Calculated by GISI) 
www.jifactor.com 
39 
 
IJARET 
© I A E M E 
STUDY THE EFFECT OF DIFFERENT OPERATING PARAMETERS ON 
HEAT TRANSFER COEFFICIENT IN GAS-SOLID FLUIDIZED BED USING 
HORIZONTAL HEAT TRANSFER PROBE 
Basma Abdulhadi Beddai1, A.V.S.S.K.S. Gupta2, M.T.Naik3, Ammar Arab Beddai4 
1Center for Energy Studies, College of Engineering, JNTUH, Kukatpally, Hyderabad, A.P 
2Mechanical Engineering, College of Engineering, JNTUH, Kukatpally, Hyderabad, A.P 
3Center for Energy Studies, College of Engineering, JNTUH, Kukatpally, Hyderabad, A.P 
4Material Engineering, Technical College- Baghdad, Iraq 
ABSTRACT 
Heat transfer studies were carried out in a laboratory scale gas-solid fluidized bed with 0.1m 
ID x 1 m length column, using three sizes of local sand particles of 301, 454, and 560 μm. the bed 
region was heated bya horizontal heat transfer probe. It was made of copper rod (15 mm ODx50 mm 
long) and insulated at the ends by Teflon. A hole was drilled at the center of the rod to accommodate 
a cartridge heater 200 W (6.5 mm OD x 42 mm long). Three bed inventories of sand 1.5 kg, 2.0 kg, 
and 2.5 kg, four superficial air velocities of 1.0 m/s, 1.25 m/s, 1.5 m/s, 1.75 m/s were used. Three 
heat fluxes of 1698.9, 2928.4, 4675.7 W m-2 were employed. The data obtained showed how the heat 
transfer coefficient effected by the above operating parameters. The heat transfer coefficient is 
directly proportional with air superficial velocity as well as the bed inventory and heat fluxes but 
inversely proportional with sand particles size. 
Keywords: Heat Transfer Coefficient, Gas- Solid Fluidized Bed, Horizontal Probe, Fluidization, 
Horizontal Probe. 
1. INTRODUCTION 
Fluidization is a unit operation, and through this technique a bed of particulate solids, 
supported over a fluid-distributing plate (often called the grid), is made to behave like a liquid by the 
passage of the fluid (gas, liquid, or gas–liquid) at a flow rate above a certain critical value. In other 
words, it is the phenomenon of imparting the properties of a fluid to a bed of particulate solids by 
passing a fluid through the latter at a velocity which brings the fixed or stationary bed to its loosest
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 
6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 
possible state just before its transformation into a fluidlike bed[1].There exist high heat transfer rate of 
fluidized beds and immersed surface, and little temperature variation across the bed, and can be 
obtained higher heat transfer coefficients compared to a conventional fluidized beds. Due to these 
advantages, this technology has been applied commercially in various processes, such as fluidized 
bed combustor, fluidized bed reactor, fluidized bed dryer, etc[2].Three modes of heat transfer are 
important with respect to surfaces immersed in fluidized beds: (1) Convection by particles carrying 
heat conducted through the gas layer in contact with the exchange surfaces; (2) convection by gas, 
and radiation. Many processes utilizing fluidized beds operate at temperatures below 500 oC where 
the radiation component is of secondary significance. Gas convective heat transfer becomes 
significant when the superficial gas velocity is higher or the particle size is large[3]. 
40 
 
Kunii and Levenspiel pointed out that heat transfer in fluidized beds is a two part concern: 
one deals with the bed to surface heat transfer such as heat transfer tubes and the other deals with the 
gas to particle heat transfer [4].Kiang et al.measured heat transfer coefficients using 19 mm diameter 
and 57.2 mm high vertical probe located along the axis at various levels in a 102-mm diameter and 
3.66-m-high cold CFB riser. Axial variation of heat transfer coefficients in the range of 45 to 230 
W/m2.K were reported. B. V. Reddy, P. K. Nag investigated the effect of operating parameters on the 
axial and radial variation of the heat transfer coefficient in circulating fluidized bed column. They 
proposed an empirical model with help of dimensional analysis to predict the heat transfer coefficient 
to a bare horizontal tube in a CFB riser column and they observed a good agreement between the 
model results and the experimental data.Noor M. Jasem et al. investigated the steady state heat 
transfer between gas and solid and the surface immersed in gas- solid CFBs. They used a bed column 
of 76 mm in inside diameter and 1500 mm in height fitted with a horizontal heating tube with outer 
diameter 28 mm heated electrically with different power supplies (105 W). The fluidizing medium 
was air at different velocities (4.97, 5.56 and 6 m/s). They employed three different size of sand 
particle (i.e 194, 295 and 356 μm). They used initial bed heights with different values (15, 25 and 35 
cm). They found that the heat transfer coefficients increase with fluidized air velocity and, through 
clear, with heat flux, but, they show an inverse dependence on particle size, and direct proportional 
with initial bed height which representation the bed density [5-7]. 
Sung Won Kim et al. carried out an experiments in a FBHE made of transparent acrylic plate. 
The effect of gas velocity on the average and local heat transfer coefficients between a submerged 
horizontal tube and a fluidized bed has been determined in a fluidized-bed-heat-exchanger of silica 
sand particles. They measured the heat transfer coefficient around the tube circumference by 
thermocouples and an optical probe. They concluded that the average heat transfer coefficient 
exhibits a maximum value with variation of gas velocity, the local heat transfer coefficient exhibits 
maximum values at the top of the tube and the average heat transfer coefficient increases with 
increasing gas velocity toward a maximum value of the coefficient[8]. 
Vanderschuren and Delvosalle (1980), Delvosalle and Vanderschuren (1985), as well as 
Molerus (1997) reported that particle–particle and particle–surface collisional heat transfers may 
play significant role in fluidized beds under certain conditions. Therefore, because of intensive 
motion of particles in the turbulent fluidized regime, it appears to be of interest of modeling and 
investigating heat transfer processes induced by particle–particle and particle–surface collisions in 
order to study these phenomena separately of the remaining thermal characteristics of the bed [9]. 
D. Karageorgieva, and R. Stanev studied the influence of some factors on total heat transfer 
coefficient and the convective heat transfer one in low temperature circulating fluidized bed. They 
compared their data with that in the literature, they found a very good agreement between them [10]. 
The heat transfer characteristics between a circulating fluidized bed and a surface immersed 
inside it were investigated by M. A. Al Busoul. He presented a statistical model describing the 
mechanism of heat transfer and the relation between the heat transfer coefficient and the main 
parameters of the bed. The proposed model yields a satisfactory representation of heat transfer
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 
6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 
process in the circulating fluidized bed.Heat transfer from an immersed heating surface to a liquid-solid 
41 
 
and liquid-liquid solid fluidized beds were studied by Balasim A. Abid et.al. The experiments 
were carried out in a (0.22) m column diameter fitted with an axially mounted cylindrical heater 
heated electrically. They developed new correlations to predict the heat transfer coefficients in 
liquid-solid and liquid-liquid-solid fluidized beds. They compared the obtained heat transfer 
coefficients with those estimated from other correlations reported in the literature. The comparison 
showed a good agreement with the data obtained for the gas-liquid-solid fluidized beds using low-density 
particles[11], [12]. 
Qin-Fu Hou, et al. investigated heat transfer characteristics of different powders in gas 
fluidization were by means of a combinedapproach of discrete element method and computational 
fluid dynamics. The results confirmed that the convective heat transfer was dominant, and radiative 
heattransfer becomes important when the bed temperature is high. However, conductive heat transfer 
also played a role depending onthe flow regimes and material properties[13]. 
Many investigations were done to study the effect of particles sizes on heat transfer 
coefficient and they obtained that the heat transfer coefficient decreases with increasing particle size 
[14-16]. 
Experiments were carried out by NimaMasoumifard, et al. in a fluidized bed in order to 
verify the influence of the axial position, particle diameter and the superficial gas velocity on the 
heat transfer coefficient from a small horizontal tube (Dt = 8 mm) immersed in the fluidized bed. The 
solid particles used were 280, 490 and 750 μm diameter sand particles, fluidized by air. They showed 
that the heat transfer coefficient was increased with increasing the gas velocity, up to a maximum, 
and then decreases with a slight slope. The heat transfer coefficient was found to decrease by 
increasing the particle size. The probe position had less influence on the heat transfer coefficients [17]. 
P. Neto et al. studied the heat transfer in a laboratory scale bubbling fluidized bed with 
54.5mm ID, using five different sizes of silica sand particles of 107.5, 142.5, 180, 282.5, and 357.5 
μm.The bubbling bed region was heated by a 2 kW electrical resistance and the heat was transfer 
towards membrane cooling wall placed above the free surface bed. They found that there were two 
heat transfer mechanisms are responsible for the thermal energy transportation towards the 
membrane cooling walls (1) the convective heat transfer from the mainly fluidized air flow, (2) the 
heat carried by the bed solid particles in the to-and-from movement created by their upward 
projection, due to the bursting bubbles reaching the bed surface, their collisions against the 
membrane walls and subsequent return to the hot bubbling bed [18].The objective of the present study 
is to investigate in detail heat transfer and to ascertain the effect of important parameters on the heat 
transfer coefficient between the horizontal heat transfer surface and the fluidized bed in a lab-scale 
fluidized bed system. 
2. EXPERIMENTAL SETUP 
Laboratory scale fluidized bed setup can be shown in fig. 1, the experiments were conducted 
in a 0.1 m ID and 1 m height mild steel fluidization column. Air was supplied by a compressor. The 
air flow was measured by a rotameter. The air was passing through the plenum chamber filled by 
glass beads to maintain uniform distribution of air through bed,with a height of 0.1m and upper 
diameter of 0.1m and bottom diameter of 0.015m. The air was distributed by a perforated plate of 
mild steel with a diameter of 0.1m and a thickness of 0.003 m will consists of 256 holes of 2.7 mm 
diameter drilled on a 7.5 mm square pitch. An ultrafine mesh was fixed on the distributor plate to 
prevent bed particles leakage. There were 10 pressure ports in the fluidized column for pressure drop 
measurements. The heat transfer section consisted from horizontal heat transfer probe.
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 
6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 
42 
 
Fig. 1: Experimental setup of fluidized bed column, 1-compressoe, 2-Valve, 3-air rotameter, 
4-plenum chamber, 5- Horizontal heat transfer probe, 6-thermocouples, 7- digital screen, 
8- DC power supply, 9-five U manometers. 
An ultrafine mesh was fixed on the top end of the column to avoid escaping the particles 
from the top. Local sand of three different sizes 301μm, 454μm, and 560 μm were used as the bed 
material. Three bed inventories of sand 1.5 kg, 2.0 kg, and 2.5 kg, four superficial air velocities of 
1.0 m/s, 1.25 m/s, 1.5 m/s, 1.75 m/s were used. Three heat fluxes of 1698.9, 2928.4, 4675.7 W m-2 
were employed. 
The local heat transfer coefficient along the probe were estimated from the equation:
(4) 
The probe average heat transfer coefficient was estimated from the local heat transfer coefficients: 
  
 
 (5) 
3. RESULTS AND DISCUSSION 
3.1 Effect of air superficial velocity on heat transfer coefficient 
Fig. 3 shows the effect of superficial gas velocity of 1.0, 1.25, 1.5, 1.75 m/s on the surface-to-bed 
heat transfer coefficient in the fluidized column at heat fluxes of 1698.9, 2928.4, 4675.7 W m-2, 
1.5 kg bed inventory and 301μm particles size. From the figure, it is noticed that the heat transfer 
coefficient increased with increasing the fluidization velocity. The increase in heat transfer may be 
due to enhanced turbulence in the column for higher velocity which in turn causes for intermixing of 
solids and gas solid suspension.
International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 
6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME
43 
 

	 

 

 

 

 


 

 
	 
 
 
 
 
 
 
Fig. 2: Effect of gas superficial velocity on heat transfer coefficient at I=1.5 kg, dp=301μm and 
three different heat fluxes 
3.2 Effect of bed inventories on heat transfer coefficient 
The effect of bed inventories on heat transfer coefficient can be shown in fig. 4. Inventory in 
the bed was varied as 1.5, 2.0, and 2.5 kg. It is observed that increase in the inventory of sand in the 
column increases the bed temperature and heat transfer coefficient. This is because sand particles 
concentration increases with increase bed inventory. Consequently, more quantity of particles in the 
lower splash region promotes more heat transfer through conduction because of which bulk 
temperature of bed was observed to be higher than that of lower inventory. W/m2 
 

 

 

 


 

 
 
 
 
Fig. 3: Effect of bed inventories on heat transfer coefficient at q=1698.9 W m-2, dp=301μm and four 
different gas superficial velocities 
 

 

 

 


 

 
 
 
Fig. 4: Effect of bed inventories on heat transfer coefficient at q=2928.4 W m-2, dp=301μm and four 
different gas superficial velocities 
h W/m2. oC 
Ug m/s 
q=1698.9 W m-2 
q=2928.4 W m-2 
q=4675.7 W m-2
h W/m2.oC 
Ug m/s 
I=1.5kg 
I=2.0kg 
I=2.5kg

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IJARET study effect operating parameters heat transfer coefficient gas-solid fluidized bed

  • 1. INTERNATIONAL JOURNAL OF ADVANCED RESEARCH International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME IN ENGINEERING AND TECHNOLOGY (IJARET) ISSN 0976 - 6480 (Print) ISSN 0976 - 6499 (Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME: http://www.iaeme.com/IJARET.asp Journal Impact Factor (2014): 7.8273 (Calculated by GISI) www.jifactor.com 39 IJARET © I A E M E STUDY THE EFFECT OF DIFFERENT OPERATING PARAMETERS ON HEAT TRANSFER COEFFICIENT IN GAS-SOLID FLUIDIZED BED USING HORIZONTAL HEAT TRANSFER PROBE Basma Abdulhadi Beddai1, A.V.S.S.K.S. Gupta2, M.T.Naik3, Ammar Arab Beddai4 1Center for Energy Studies, College of Engineering, JNTUH, Kukatpally, Hyderabad, A.P 2Mechanical Engineering, College of Engineering, JNTUH, Kukatpally, Hyderabad, A.P 3Center for Energy Studies, College of Engineering, JNTUH, Kukatpally, Hyderabad, A.P 4Material Engineering, Technical College- Baghdad, Iraq ABSTRACT Heat transfer studies were carried out in a laboratory scale gas-solid fluidized bed with 0.1m ID x 1 m length column, using three sizes of local sand particles of 301, 454, and 560 μm. the bed region was heated bya horizontal heat transfer probe. It was made of copper rod (15 mm ODx50 mm long) and insulated at the ends by Teflon. A hole was drilled at the center of the rod to accommodate a cartridge heater 200 W (6.5 mm OD x 42 mm long). Three bed inventories of sand 1.5 kg, 2.0 kg, and 2.5 kg, four superficial air velocities of 1.0 m/s, 1.25 m/s, 1.5 m/s, 1.75 m/s were used. Three heat fluxes of 1698.9, 2928.4, 4675.7 W m-2 were employed. The data obtained showed how the heat transfer coefficient effected by the above operating parameters. The heat transfer coefficient is directly proportional with air superficial velocity as well as the bed inventory and heat fluxes but inversely proportional with sand particles size. Keywords: Heat Transfer Coefficient, Gas- Solid Fluidized Bed, Horizontal Probe, Fluidization, Horizontal Probe. 1. INTRODUCTION Fluidization is a unit operation, and through this technique a bed of particulate solids, supported over a fluid-distributing plate (often called the grid), is made to behave like a liquid by the passage of the fluid (gas, liquid, or gas–liquid) at a flow rate above a certain critical value. In other words, it is the phenomenon of imparting the properties of a fluid to a bed of particulate solids by passing a fluid through the latter at a velocity which brings the fixed or stationary bed to its loosest
  • 2. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME possible state just before its transformation into a fluidlike bed[1].There exist high heat transfer rate of fluidized beds and immersed surface, and little temperature variation across the bed, and can be obtained higher heat transfer coefficients compared to a conventional fluidized beds. Due to these advantages, this technology has been applied commercially in various processes, such as fluidized bed combustor, fluidized bed reactor, fluidized bed dryer, etc[2].Three modes of heat transfer are important with respect to surfaces immersed in fluidized beds: (1) Convection by particles carrying heat conducted through the gas layer in contact with the exchange surfaces; (2) convection by gas, and radiation. Many processes utilizing fluidized beds operate at temperatures below 500 oC where the radiation component is of secondary significance. Gas convective heat transfer becomes significant when the superficial gas velocity is higher or the particle size is large[3]. 40 Kunii and Levenspiel pointed out that heat transfer in fluidized beds is a two part concern: one deals with the bed to surface heat transfer such as heat transfer tubes and the other deals with the gas to particle heat transfer [4].Kiang et al.measured heat transfer coefficients using 19 mm diameter and 57.2 mm high vertical probe located along the axis at various levels in a 102-mm diameter and 3.66-m-high cold CFB riser. Axial variation of heat transfer coefficients in the range of 45 to 230 W/m2.K were reported. B. V. Reddy, P. K. Nag investigated the effect of operating parameters on the axial and radial variation of the heat transfer coefficient in circulating fluidized bed column. They proposed an empirical model with help of dimensional analysis to predict the heat transfer coefficient to a bare horizontal tube in a CFB riser column and they observed a good agreement between the model results and the experimental data.Noor M. Jasem et al. investigated the steady state heat transfer between gas and solid and the surface immersed in gas- solid CFBs. They used a bed column of 76 mm in inside diameter and 1500 mm in height fitted with a horizontal heating tube with outer diameter 28 mm heated electrically with different power supplies (105 W). The fluidizing medium was air at different velocities (4.97, 5.56 and 6 m/s). They employed three different size of sand particle (i.e 194, 295 and 356 μm). They used initial bed heights with different values (15, 25 and 35 cm). They found that the heat transfer coefficients increase with fluidized air velocity and, through clear, with heat flux, but, they show an inverse dependence on particle size, and direct proportional with initial bed height which representation the bed density [5-7]. Sung Won Kim et al. carried out an experiments in a FBHE made of transparent acrylic plate. The effect of gas velocity on the average and local heat transfer coefficients between a submerged horizontal tube and a fluidized bed has been determined in a fluidized-bed-heat-exchanger of silica sand particles. They measured the heat transfer coefficient around the tube circumference by thermocouples and an optical probe. They concluded that the average heat transfer coefficient exhibits a maximum value with variation of gas velocity, the local heat transfer coefficient exhibits maximum values at the top of the tube and the average heat transfer coefficient increases with increasing gas velocity toward a maximum value of the coefficient[8]. Vanderschuren and Delvosalle (1980), Delvosalle and Vanderschuren (1985), as well as Molerus (1997) reported that particle–particle and particle–surface collisional heat transfers may play significant role in fluidized beds under certain conditions. Therefore, because of intensive motion of particles in the turbulent fluidized regime, it appears to be of interest of modeling and investigating heat transfer processes induced by particle–particle and particle–surface collisions in order to study these phenomena separately of the remaining thermal characteristics of the bed [9]. D. Karageorgieva, and R. Stanev studied the influence of some factors on total heat transfer coefficient and the convective heat transfer one in low temperature circulating fluidized bed. They compared their data with that in the literature, they found a very good agreement between them [10]. The heat transfer characteristics between a circulating fluidized bed and a surface immersed inside it were investigated by M. A. Al Busoul. He presented a statistical model describing the mechanism of heat transfer and the relation between the heat transfer coefficient and the main parameters of the bed. The proposed model yields a satisfactory representation of heat transfer
  • 3. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME process in the circulating fluidized bed.Heat transfer from an immersed heating surface to a liquid-solid 41 and liquid-liquid solid fluidized beds were studied by Balasim A. Abid et.al. The experiments were carried out in a (0.22) m column diameter fitted with an axially mounted cylindrical heater heated electrically. They developed new correlations to predict the heat transfer coefficients in liquid-solid and liquid-liquid-solid fluidized beds. They compared the obtained heat transfer coefficients with those estimated from other correlations reported in the literature. The comparison showed a good agreement with the data obtained for the gas-liquid-solid fluidized beds using low-density particles[11], [12]. Qin-Fu Hou, et al. investigated heat transfer characteristics of different powders in gas fluidization were by means of a combinedapproach of discrete element method and computational fluid dynamics. The results confirmed that the convective heat transfer was dominant, and radiative heattransfer becomes important when the bed temperature is high. However, conductive heat transfer also played a role depending onthe flow regimes and material properties[13]. Many investigations were done to study the effect of particles sizes on heat transfer coefficient and they obtained that the heat transfer coefficient decreases with increasing particle size [14-16]. Experiments were carried out by NimaMasoumifard, et al. in a fluidized bed in order to verify the influence of the axial position, particle diameter and the superficial gas velocity on the heat transfer coefficient from a small horizontal tube (Dt = 8 mm) immersed in the fluidized bed. The solid particles used were 280, 490 and 750 μm diameter sand particles, fluidized by air. They showed that the heat transfer coefficient was increased with increasing the gas velocity, up to a maximum, and then decreases with a slight slope. The heat transfer coefficient was found to decrease by increasing the particle size. The probe position had less influence on the heat transfer coefficients [17]. P. Neto et al. studied the heat transfer in a laboratory scale bubbling fluidized bed with 54.5mm ID, using five different sizes of silica sand particles of 107.5, 142.5, 180, 282.5, and 357.5 μm.The bubbling bed region was heated by a 2 kW electrical resistance and the heat was transfer towards membrane cooling wall placed above the free surface bed. They found that there were two heat transfer mechanisms are responsible for the thermal energy transportation towards the membrane cooling walls (1) the convective heat transfer from the mainly fluidized air flow, (2) the heat carried by the bed solid particles in the to-and-from movement created by their upward projection, due to the bursting bubbles reaching the bed surface, their collisions against the membrane walls and subsequent return to the hot bubbling bed [18].The objective of the present study is to investigate in detail heat transfer and to ascertain the effect of important parameters on the heat transfer coefficient between the horizontal heat transfer surface and the fluidized bed in a lab-scale fluidized bed system. 2. EXPERIMENTAL SETUP Laboratory scale fluidized bed setup can be shown in fig. 1, the experiments were conducted in a 0.1 m ID and 1 m height mild steel fluidization column. Air was supplied by a compressor. The air flow was measured by a rotameter. The air was passing through the plenum chamber filled by glass beads to maintain uniform distribution of air through bed,with a height of 0.1m and upper diameter of 0.1m and bottom diameter of 0.015m. The air was distributed by a perforated plate of mild steel with a diameter of 0.1m and a thickness of 0.003 m will consists of 256 holes of 2.7 mm diameter drilled on a 7.5 mm square pitch. An ultrafine mesh was fixed on the distributor plate to prevent bed particles leakage. There were 10 pressure ports in the fluidized column for pressure drop measurements. The heat transfer section consisted from horizontal heat transfer probe.
  • 4. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 42 Fig. 1: Experimental setup of fluidized bed column, 1-compressoe, 2-Valve, 3-air rotameter, 4-plenum chamber, 5- Horizontal heat transfer probe, 6-thermocouples, 7- digital screen, 8- DC power supply, 9-five U manometers. An ultrafine mesh was fixed on the top end of the column to avoid escaping the particles from the top. Local sand of three different sizes 301μm, 454μm, and 560 μm were used as the bed material. Three bed inventories of sand 1.5 kg, 2.0 kg, and 2.5 kg, four superficial air velocities of 1.0 m/s, 1.25 m/s, 1.5 m/s, 1.75 m/s were used. Three heat fluxes of 1698.9, 2928.4, 4675.7 W m-2 were employed. The local heat transfer coefficient along the probe were estimated from the equation:
  • 5. (4) The probe average heat transfer coefficient was estimated from the local heat transfer coefficients: (5) 3. RESULTS AND DISCUSSION 3.1 Effect of air superficial velocity on heat transfer coefficient Fig. 3 shows the effect of superficial gas velocity of 1.0, 1.25, 1.5, 1.75 m/s on the surface-to-bed heat transfer coefficient in the fluidized column at heat fluxes of 1698.9, 2928.4, 4675.7 W m-2, 1.5 kg bed inventory and 301μm particles size. From the figure, it is noticed that the heat transfer coefficient increased with increasing the fluidization velocity. The increase in heat transfer may be due to enhanced turbulence in the column for higher velocity which in turn causes for intermixing of solids and gas solid suspension.
  • 6. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME
  • 7. 43 Fig. 2: Effect of gas superficial velocity on heat transfer coefficient at I=1.5 kg, dp=301μm and three different heat fluxes 3.2 Effect of bed inventories on heat transfer coefficient The effect of bed inventories on heat transfer coefficient can be shown in fig. 4. Inventory in the bed was varied as 1.5, 2.0, and 2.5 kg. It is observed that increase in the inventory of sand in the column increases the bed temperature and heat transfer coefficient. This is because sand particles concentration increases with increase bed inventory. Consequently, more quantity of particles in the lower splash region promotes more heat transfer through conduction because of which bulk temperature of bed was observed to be higher than that of lower inventory. W/m2 Fig. 3: Effect of bed inventories on heat transfer coefficient at q=1698.9 W m-2, dp=301μm and four different gas superficial velocities Fig. 4: Effect of bed inventories on heat transfer coefficient at q=2928.4 W m-2, dp=301μm and four different gas superficial velocities h W/m2. oC Ug m/s q=1698.9 W m-2 q=2928.4 W m-2 q=4675.7 W m-2
  • 8. h W/m2.oC Ug m/s I=1.5kg I=2.0kg I=2.5kg
  • 9. h W/m2.oC Ug m/s I=1.5kg I=2.0kg I=2.5kg
  • 10. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 300 280 260 240 220 200 180 160 0.95 1.15 1.35 1.55 1.75 1.95 Fig. 5: Effect of bed inventories on heat transfer coefficient at q=4675.7 W m-2, dp=301μm and four 44 different gas superficial velocities 3.3 Effect of sand particle size on heat transfer coefficient Fig. 7, 8, and 9 show the effect of particle size on the heat transfer coefficient between the heat transfer probe and the bed particles. Sand particles size of 301, 454, and 560 μm were used.It is found that the heat transfer coefficient decreases for large particles mainly because of the higher thermal resistance offered by the particles. Also with increase of particle size, the gas gap thickness between the surface and particles increases resulting in a decrease of the heat transfer coefficient. Moreover the smaller particles can increase the effective heat transfer area covered by particle itself. 220 200 180 160 140 120 Fig. 6: Effect of particles size on heat transfer coefficient at q=1698.9 W m-2, I=1.5 kg, and four different gas superficial velocities 280 260 240 220 200 180 160 140 120 Fig. 7: Effect of particles size on heat transfer coefficient at q=2928.4 W m-2, I=1.5 kg, and four different gas superficial velocities h W/m2.oC Ug m/s I=1.5kg I=2.0kg I=2.5kg 100 0.9 1.1 1.3 1.5 1.7 1.9 h W/m2.oC Ug m/s dp=301μm dp=450μm dp=560μm 100
  • 12. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 0.9 1.1 1.3 1.5 1.7 1.9 45 300 280 260 240 220 200 180 160 140 120 100 h W/m2.oC Ug m/s dp=301μm dp=450μm dp=560μm Fig. 8: Effect of particles size on heat transfer coefficient at q=4675.7 W m-2, I=1.5 kg, and four different gas superficial velocities 3.4 Effect of heat fluxes on heat transfer coefficient The variation of heat transfer coefficient for different heat flux conditions against gas superficial velocity for a particular bed inventory is shown in fig. 3. The heat transfer coefficient is high for higher values of heat flux and it is decreasing with the decrease in heat flux. For higher heat flux condition, the bed temperature increases. This is due to increase of amount of the heat which transferred to the fluidized bed system, which in turn tends to enhance the heat transfer coefficient. 4. CONCLUSIONS The main focus of this study was the effect of different operating parameters on heat transfer coefficient in gas-solid fluidized bed. Following conclusions obtained from the experimental results: 1. Heat transfer coefficient is found to be increasing with increase air superficial velocity. 2. Heat transfer coefficient is directly proportional to the heat fluxes and bed inventory. 3. Smaller particles size yield higher heat transfer coefficient and vice versa in present heat transfer studies. 4. The data show trends similar to those in published literatures. REFERENCES [1.] C.K. Gupta, D. Sathiyamoorthy, Fluid Bed Technology in Materials Processing, 1999 by CRC Press LLC. [2.] Zhu Xuejun, Ye Shichao, Pan Xiaoheng, The local heat transfer mathematical model between vibrated fluidized beds and horizontal tubes, Experimental Thermal and Fluid Science 32 (2008) 1279–1286. [3.] A. Stefanova, H.T. Bi, C.J. Lim, J.R. Grace, Heat transfer from immersed vertical tube in a fluidized bed of group A particles near the transition to the turbulent fluidization flow regime, International Journal of Heat and Mass Transfer 51 (2008) 2020–2028. [4.] K. Pisters, A. Prakash, Investigations of axial and radial variations of heat transfer coefficient in bubbling fluidized bed with fast response probe, Powder Technology 207 (2011) 224–231. [5.] R. Sundaresan, Ajit Kumar Kolar Core heat transfer studies in a circulating fluidized bed Powder Technology 124 (2002) 138– 151. [6.] B. V. Reddy, P. K. Nag, Axial And Radial Heat Transfer Studies in a Circulating Fluidized Bed, International Journal of Energy Research, VOL. 21, 1109-1122 (1997).
  • 13. International Journal of Advanced Research in Engineering and Technology (IJARET), ISSN 0976 – 6480(Print), ISSN 0976 – 6499(Online) Volume 5, Issue 7, July (2014), pp. 39-46 © IAEME 46 [7.] Noor M. Jasem, GhassanFadhil. M. H., Hafidh H. Mohammed, Experimental Study Of The Effect Bed Density On Heat Transfer Coefficients In Towers With Gas Solid Circulating Fluidized Bed, Al-Qadisiya Journal For Engineering Sciences 2009 Vol. 2 No. 3. [8.] Anusaya M. Salwe, Local heat transfer coefficient around a horizontal heating element in gas-solid fluidized bed, International Journal of Application or Innovation in Engineering Management (IJAIEM), Volume 2, Issue 6, June 2013 ISSN 2319 – 4847. [9.] Z. Sule, B.G. Lakatos, Cs. Mihalyko, Axial dispersion/population balance model of heat transfer in gas–solid turbulent fluidized beds, Computers and Chemical Engineering 34 (2010) 753–762. [10.] D. Karageorgieva, R. Stanev, Heat Transfer in Low Temperature Circulating Fluidized Bed, Journal of the University of Chemical Technology and Metallurgy, 41, 1, 2006, 69-74. [11.] M. A. Al Busoul, Bed- to- Surface Heat Transfer Coefficient ion Circulating Fluidized Bed, heat and mass transfer 38 (2002) 295-299. [12.] Balasim A. Abid, Majid I. Abdul-Wahab, Asrar A. Al-Obaidy, Heat Transfer from an Immersed Heater in Liquid – Liquid – Solid Fluidized Beds, Eng. Tech. Journal, 2009 Vol.27, No.10. [13.] Qin-Fu Hou, Zong-Yan Zhou, Ai-Bing Yu, Computational Study of the Effects of Material Properties on Heat Transfer in Gas Fluidization, Industrial Engineering Chemistry Research 2012, 51, 11572−11586. [14.] A.V.S.S.Kumara Swami Gupta, Some Heat Transfer and Thermodynamic Studies of Combined Cycle Power Generation, Thesis 1999. [15.] JamalMane'e Al-Rubeai, Nabeel Majid Aliwi, A Study of Chaotic Behavior of Heat Transfer In Gas-SolidFluidized Bed, Eng. Tech. Journal, Vol.28, 2010, No.10. [16.] Tahseen Al-Hattb and Riyadh S. Al-Turhee, Effect of Particle Size,Flow Velocity And Heat Flux on Heat Transfer Coefficient in Fluidized Bed Column, The Iraqi Journal For Mechanical And Material Engineering, Special Issue (B). [17.] NimaMasoumifard, NavidMostoufi*, Ali-AsgharHamidi, RahmatSotudeh-Gharebagh, Investigation of Heat Transfer between a Horizontal Tube and Gas–Solid Fluidized Bed, International Journal of Heat and Fluid Flow 29 (2008) 1504–1511. [18.] P. Neto, A. M. Ribeiro, C. Pinho, Heat Transfer abovethe Free Surface ofa Bubbling Fluidized Bed: A Simple Global Correlation, International Review of Chemical Engineering, Vol. 1, 2009, N.1. [19.] Mamdoh Al-Busoul, Aiman Al-Alawin and Hamza Al-Tahaineh, “Influence of Air-Fuel Ratio and Particle Size on Fluidized Bed Combustion of the El-Lajjun Oil Shale”, International Journal of Mechanical Engineering Technology (IJMET), Volume 4, Issue 5, 2013, pp. 130 - 138, ISSN Print: 0976 – 6340, ISSN Online: 0976 – 6359. [20.] M. Sreekanth, “Measurement of Devolatilization Time and Transient Shrinkage of a Cylindrical Wood Particle in a Bubbling Fluidized Bed Combustor”, International Journal of Mechanical Engineering Technology (IJMET), Volume 4, Issue 3, 2013, pp. 244 - 258, ISSN Print: 0976 – 6340, ISSN Online: 0976 – 6359. [21.] Phairoach Chunkaew, Aree Achariyaviriya, Siva Achariyaviriya, James C. Moran and Sujinda Sriwattana, “Operating Parameters Effects on Drying Kinetics and Salted Sunflower Seed Quality Utilizing a Fluidized Bed”, International Journal of Advanced Research in Engineering Technology (IJARET), Volume 4, Issue 6, 2013, pp. 256 - 268, ISSN Print: 0976-6480, ISSN Online: 0976-6499.