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SIMULATION OF CONJUGATE HEAT TRANSFER AND NATURAL CONVECTION IN THE UNFILLED CAVITY-WALLS OF BUILDING USING ADINA-CFD ANIL KUMAR PATIDAR 1 , RAMESH KANNAN.M 2 1 PG Student, 2 Assistant Professor, 1,2 Department of Civil Engineering, School of Mechanical and Building Sciences, VIT Chennai, Tamil Nadu, India ABSTRACT This paper deals with the simulation of conjugate heat transfer and natural convection phenomenon in different cavity walls and its effect on the thermal insulation of building. The simulations are carried out by creation of preliminary models in CAD and detailed models with the desired boundary conditions in ADINA-CFD and analyzed for the heat transfer and heat movement inside the cavity present between various wall materials, commonly used in cavity walls. The type of simulation adopted for this research is the Heat transport simulation using Heatline Visualization Technique and the heat barrier effect. This paper also focuses on the comparison of emprical values on the conjugate heat transfer and natural convection of cavity walls with the simulation result. From the litertaure, the effect of heat barrier location on overall heat transfer is large for low Rayleigh number cavities. The average Nusselt number also reduces with the due to the heat barrier. These characteristics are well observed in the conducted simulation and from the simulation, the wall cavity with Wood and Brick configuration is proved to be best material combination for the cavity walls for thermal insulations. KEYWORDS: ADINA-CFD, conjugate energy efficiency, heat transfer, heatline visualization technique, natural convection, Rayleigh number. INTRODUCTION A cavity wall is two walls of masonry construction separated by an air cavity. The cavities range from 2" to 4.5" thick. The effect of wall heat conduction on natural convection heat transfer in cavities has gained attention of many researchers in recent years due to its wide application areas in engineering such as buildings cooling and heating, thick-walled enclosures, cooling of electronic equipments, solar collectors and cooling of internal combustion engines. More heat is lost through the walls of buildings than in any other way. Up to 35% of domestic heat is wasted across un-insulated cavity walls, which means that consuming energy far in excess of our requirements. Many researchers have performed several numerical and experimental studies on natural convection to investigate the effect of wall heat conduction on heat transfer. De Vahl Davis (1983) concluded that the computational method has been used to obtain accurate numerical solutions of the equations describing 2-D natural convection heat of transfer in a square cavity. Kaminski et al. (1986) investigated the conjugate natural convection problem in the enclosure with one thick vertical wall. Acharya et al. (1987) conducted a numerical study on natural convection in an externally heated inclined enclosure with finitely conducting side walls. The result indicates
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Simulation of Conjugate Heat Transfer and Natural Convection

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Simulation of Conjugate Heat Transfer and Natural Convection
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  • SIMULATION OF CONJUGATE HEAT TRANSFER AND NATURAL CONVECTION

    IN THE UNFILLED CAVITY-WALLS OF BUILDING USING ADINA-CFD

    ANIL KUMAR PATIDAR1, RAMESH KANNAN.M

    2

    1PG Student,

    2Assistant Professor,

    1,2Department of Civil Engineering, School of Mechanical and Building Sciences, VIT Chennai, Tamil Nadu, India

    ABSTRACT

    This paper deals with the simulation of conjugate heat transfer and natural convection phenomenon in

    different cavity walls and its effect on the thermal insulation of building. The simulations are carried out by creation

    of preliminary models in CAD and detailed models with the desired boundary conditions in ADINA-CFD and

    analyzed for the heat transfer and heat movement inside the cavity present between various wall materials,

    commonly used in cavity walls. The type of simulation adopted for this research is the Heat transport simulation

    using Heatline Visualization Technique and the heat barrier effect. This paper also focuses on the comparison of

    emprical values on the conjugate heat transfer and natural convection of cavity walls with the simulation result.

    From the litertaure, the effect of heat barrier location on overall heat transfer is large for low Rayleigh number

    cavities. The average Nusselt number also reduces with the due to the heat barrier. These characteristics are well

    observed in the conducted simulation and from the simulation, the wall cavity with Wood and Brick configuration is

    proved to be best material combination for the cavity walls for thermal insulations.

    KEYWORDS: ADINA-CFD, conjugate energy efficiency, heat transfer, heatline visualization technique, natural

    convection, Rayleigh number.

    INTRODUCTION

    A cavity wall is two walls of masonry construction separated by an air cavity. The cavities range from 2" to

    4.5" thick. The effect of wall heat conduction on natural convection heat transfer in cavities has gained attention of

    many researchers in recent years due to its wide application areas in engineering such as buildings cooling and

    heating, thick-walled enclosures, cooling of electronic equipments, solar collectors and cooling of internal

    combustion engines. More heat is lost through the walls of buildings than in any other way. Up to 35% of domestic

    heat is wasted across un-insulated cavity walls, which means that consuming energy far in excess of our

    requirements.

    Many researchers have performed several numerical and experimental studies on natural convection to

    investigate the effect of wall heat conduction on heat transfer. De Vahl Davis (1983) concluded that the

    computational method has been used to obtain accurate numerical solutions of the equations describing 2-D natural

    convection heat of transfer in a square cavity. Kaminski et al. (1986) investigated the conjugate natural convection

    problem in the enclosure with one thick vertical wall. Acharya et al. (1987) conducted a numerical study on

    natural convection in an externally heated inclined enclosure with finitely conducting side walls. The result indicates

  • the reduction of heat transfer from the enclosure. Du et al. (1992) studied conjugate heat transfer in an enclosure

    which consists of a conducting vertical wall of finite thickness with a uniform heat input and an insulated vertical

    wall and two horizontal walls at a heat sink temperature.

    Baytas et al. (2002) studied the steady-state conjugate natural convection in a square cavity filled with a

    porous medium which consists of two horizontal conductive walls of finite thickness and two vertical walls at

    different uniform temperatures. Hakyemez et al. (2008) has investigated the effects of wall-located heat barrier on

    conjugate conduction and natural convection heat transfer and fluid flow in enclosures.

    The major benefits of cavity walls vary from short term benefits to long term benefits. Some of the major

    short term and long term benefits are as follows.

    1. All materials required are locally available hence reducing the transportation cost

    2. Limited craft work reduces the construction time which in turn results in savings due to early occupancy

    3. Energy efficiency of a building increases due to cavity wall construction

    4. On the long term, masonry construction is very economical

    TYPES OF CAVITY WALL

    Cavity walls ranges from simple masonry-masonry wall to sophisticated concrete-metallic walls depending

    upon of the requirements, thermal comfort and other related factors. Cavity walls can also be categorized into

    unfilled and in-filled cavity wall. Unfilled cavity walls are the normal walls whereas the in-filled are special types,

    which consider the incorporation of insulating materials for enhanced thermal resistance of the wall. The commonly

    used types of cavity walls are as shown in Fig 1.

    The unfilled cavity walls exhibits satisfactory thermal insulating properties such as natural convection and

    heat transfer phenomenon than the in-filled walls, moreover by swapping the materials of interior and exterior walls,

    we would get different patterns of convection and heat transfer.

    (a) (b)

    Figure 1. Typical (a). Brick - Brick unfilled cavity wall, (b). Brick Concrete, foam- filed cavity wall

    RESEARCH METHODOLOGY

    The basic assumptions and the detailed methodology adopted for this research are as follows:

  • The important assumptions made for this project are listed below:

    1. The cavity wall considered is a unfilled cavity wall types, since the heat transfer cannot be visualized by

    the in-filled cavity walls

    2. The wall thickness for both interior and exterior walls is kept constant; the specified wall thickness

    considered for brick is 250mm (without plaster) and concrete, timber (wood), metallic wall (steel) is

    250mm.

    3. The length of cavity wall taken for simulation is 1.00 m length and 3.00 m height

    4. The cavity wall is considered to be a sealed cavity wall, the top, bottom and sides are closed for the

    visualization of the heat transfer.

    5. The materials used in the cavity walls (Interior Exterior walls) considered in this research are as follows:

    Brick Brick cavity wall, Brick Concrete cavity wall, Brick Wood cavity wall, Brick Steel cavity

    wall, Concrete Brick cavity wall, Concrete Concrete cavity wall, Concrete Wood cavity wall,

    Concrete Steel cavity wall, Wood Brick cavity wall, Wood Concrete cavity wall, Wood wood

    cavity wall, Wood Steel Concrete Wall, Steel Brick cavity wall, Steel Concrete cavity wall, Steel -

    Wood cavity wall, Steel Steel cavity wall. The detailed explain of the cavity walls used in this research

    are illustrated in the Fig 2.

    Figure 2. Matrix of Cavity Walls with different interior and exterior walls

  • The conceptual framework of this research is as follows:

    Figure 3. Research Methodology flowchart.

    NUMERICAL FORMULATION OF NATURAL CONVECTION AND CONJUGATE HEAT

    TRANSFER

    The most common measure of thermal performance of a building material is R-value. An R-value is a

    measure of the thermal resistance of a material. The use of single number is convenient and easily understood. The

    R-value is only a measure of the materials` ability to insulate. The R-value is not the complete measure of materials

    thermal performance. Thermal mass cannot be easily measured, but is easily found in dense materials like bricks. It

    is important to remember that a proper combination of both insulation and thermal mass will create a well designed

    home.

    Brickwork due to its high bulk density has a corresponding large thermal capacity with its ability to absorb

    and store significant quantity of heat during daytime increasing temperature and to isolate this heat in a controlled

    manner during periods of right time decreasing temperature.

    The R-value is a measure of thermal resistance used in the building industry. Under standard conditions it is

    the ratio of the temperature difference across an insulator and the heat flux. Heat Flux is the heat transfer per unit

    area per unit time through it.

  • The local and average Nusselt numbers for the vertical walls of the fluid region are calculated according to

    the gradient of dimensionless temperature in the normal direction of the considered wall. For the hot and cold

    vertical walls of the cavity (X=0, X=1) are calculated by the following equations.

    Nu = qfL / Kf (Th-Tc) = f / Xwall 1.

    Nu = 1

    0 2.

    The dimensionless heat transfer rate from a wall of the fluid region can be calculated as.

    Q*f =

    1

    0f / Xwall dY 3.

    The dimensionless heat flux and heat transfer rate, q*

    s and Q*s , from the vertical boundaries of the horizontal wall

    can be calculated by the following relations.

    q*s = qs L / ks (Th Tc) = s / Xwall 4.

    Q*s = s / Xwall dY

    1+

    1 5.

    The dimensionless overall heat transfer rate to/from the entire area of the hot or cold vertical wall can be calculated

    by the following equation.

    Q*t = Q

    *s K + Q

    *f 6.

    Where,

    n = refer to (n+1)th

    time step, n = refer to nth

    time step, q* = dimensionless heat flux, Q* = dimensionless heat

    transfer rate, Nu = local Nusselt number, Nu = average Nusselt number

  • SIMULATION OF CONJUGATE HEAT TRANSFER AND NATURAL CONVECTION IN THE

    CAVITY WALLS

    The detailed procedure and description of boundary-condition and messing of cavity wall in ADINA-CFD

    are given in Fig 4.(a)-(c).

    (a) (b) (c)

    Figure 4. (a) Setting up of boundary conditions (b) Meshing of the cavity wall (c) Setting up of particle trace steady

    flow time and path line

  • RESULTS AND DISCUSSIONS

    The heat flux, value from the simulations is tabulated in Tab 3. The values are plotted in a graph with

    Cavity wall along X-Axis and Heat Flux along Y-axis as shown in Fig 21.

    Figure 21. Heat flux values of different cavity walls.

    From the above figure and table, we infer that Wood-Wood has the least radiant flux, thus it produces lot of

    thermal comfort during the later stage or night. However, for the practical point of Brick-Wood combination is

    effective in energy efficient as well moisture control or performance of the building itself. To rank to three cavity

    wall combinations are: Brick-Wood, Brick-Concrete and Wood-Wood.

  • CONCLUSIONS

    From the results obtained from the simulation, we conclude that the cavity wall helps in the overall heat

    transfer in a room and also helps to reduce the energy consumption of the building. The best combination of

    materials for cavity wall construction is Brick Wood combination. This combination gave us the highest

    temperature range amongst the various material combinations tested. The next best combination was found to be that

    of Wood Concrete cavity wall. The usage of wood is not possible in all the areas, in that cases, the Brick Brick

    cavity wall yields satisfactory performance. The cavity wall is not only useful for cold regions but also for hotter

    regions, as it reduces the heat induction through the walls into the building and hence acts as radiant barriers.

    REFERENCES

    1. Acharya, S. and Tsang, C.H. 1987. Influence of wall conductivity on natural convection sq. enclosure. Heat

    and Mass Transfer 21: 19-30.

    2. Baytas, A.C., Liaqat, A. and Grosan, T. 2001. Conjugate natural convection in a square porous cavity.

    Heat and Mass Transfer 37:467-473.

    3. De Vahl Davis, G. 1983. Natural convection of air in a square cavity. International Journal of Numerical

    Methods in Fluids 3: 249-264.

    4. Du, Z.G. and Bilgen, E. 1992. Coupling of wall conductivity with natural convection during a rectangular

    enclosure. International Journal of Heat and Mass Transfer 35: 1962-1975.

    5. Hakyemez, E., Mobedi, M. and Oztop, H.F. 2008. Effects of wall- located heat barrier on conjugate

    conduction and natural convection heat transfer and fluid flow in enclosures. Numerical Heat Transfer 54:

    197220.

    6. Kaminski, D.A. and Prakash, C. 1986. Conjugate natural convection problem in the enclosure with one

    thick vertical wall. International Journal of Heat and Mass Transfer 12: 1979-1988.

    7. Kim, D.M. and Viskanta, R. 1984. Effects of wall conductance on natural convection in differently oriented

    cavities. Journal of Fluid Mechanics 144: 153-176.

    8. Misra, D. and Sarkar, A. 1997. Finite component analysis of conjugate natural convection during a

    square enclosure with a conducting vertical wall with totally different temperature. Computer Methods in

    Applied Mechanics and Engineering 141: 205-219.

    9. Yedder, R.B.and Bilgen, E. 1997. Heat barrier on conjugate conduction and natural convection heat

    transfer and fluid flow in enclosures. Heat and Mass Transfer 32: 455-462.