Modeling Superheated Steam Vacuum Drying of Wood

Abstract A two-dimensional mathematical model developed for vacuum-contact drying of wood was adapted to simulate superheated steam vacuum drying. The moisture and heat equations are based on the water potential concept whereas the pressure equation is formulated considering unsteady-state mass conservation of dry air. A drying test conducted on sugar maple sapwood in a laboratory vacuum kiln was used to infer the convective mass and heat transfer coefficients through a curve fitting technique. The average air velocity was 2.5 m s−1 and the dry-bulb temperature varied between 60 and 66°C. The ambient pressure varied from 15 to 11 kPa. Simulation results indicate that heat and mass transfer coefficients are moisture content dependent. The simulated drying curve based on transfer coefficients calculated from boundary layer theory poorly fits experimental results. The functional relation for the relative permeability of wood to air is a key parameter in predicting the pressure evolution in wood in the course of drying. In the case of small vacuum kilns, radiant heat can contribute substantially to the total heat transfer to the evaporative surface at the early stages of drying. As for conventional drying, the air velocity could be reduced at the latter stage of drying with little or no change to the drying rate.

[1]  A. Degiovanni,et al.  Simulation par volumes finis des transferts couplés en milieux poreux anisotropes : séchage du bois à basse et à haute température , 1990 .

[2]  Alain Cloutier,et al.  MODELING VACUUM-CONTACT DRYING OF WOOD: THE WATER POTENTIAL APPROACH , 2000 .

[3]  W. Jomaa,et al.  DISCONTINUOUS VACUUM DRYING OF OAK WOOD: MODELLING AND EXPERIMENTAL INVESTIGATIONS , 1997 .

[4]  A. V. Luikov,et al.  CHAPTER 6 – HEAT AND MASS TRANSFER IN CAPILLARY-POROUS BODIES , 1966 .

[5]  John F. Siau,et al.  Wood--influence of moisture on physical properties , 1995 .

[6]  S. Whitaker Simultaneous Heat, Mass, and Momentum Transfer in Porous Media: A Theory of Drying , 1977 .

[7]  I. Turner,et al.  An investigation of the boundary conditions for a vacuum drying problem--introducing the transition layer concept , 1994 .

[8]  A. Hukka,et al.  The Effective Diffusion Coefficient and Mass Transfer Coefficient of Nordic Softwoods as Calculated from Direct Drying Experiments , 1999 .

[9]  Y. Fortin,et al.  Moisture Content-Water Potential Relationship of Sugar Maple and White Spruce Wood From Green to Dry Conditions , 1999 .

[10]  C. Moyne,et al.  Etude experimentale du transfert simultane de chaleur et de masse au cours du sechage par contact sous vide d'un bois resineux , 1982 .

[11]  Alain Cloutier,et al.  Experimental determination of the convective heat and mass transfer coefficients for wood drying , 2000, Wood Science and Technology.

[12]  William T. Simpson,et al.  Predicting Equilibrium Moisture Content of Wood by Mathematical Models , 1973 .

[13]  Y. Fortin,et al.  Determination of the Effective Water Conductivity of Sugar Maple Sapwood and White Spruce Heartwood Under Vacuum , 1999 .

[14]  Stig Stenström,et al.  Evaluation of Equations Approximating Thermodynamic and Transport Properties of Water, Steam and Air for Use in CAD of Drying Processes , 1991 .

[15]  A. Hanhijärvi,et al.  Experimental investigation of jet drying of birch and spruce veneers and modelling with a simplified approach , 2003, Holz als Roh- und Werkstoff.

[16]  S. Pang RELATIVE IMPORTANCE OF VAPOUR DIFFUSION AND CONVECTTVE FLOW IN MODELLING OF SOFTWOOD DRYING , 1998 .

[17]  Frank P. Incropera,et al.  Fundamentals of Heat and Mass Transfer , 1981 .

[18]  Jarl-Gunnar Salin Prediction of heat and mass transfer coefficients for individual boards and board surfaces. A review. Paper presented at the 5th International IUFRO wood drying conference, Quebec City, Canada, August 13-17, 1996 , 1997 .