Abstract
A new approach to experimental evaluation of mass transfer resistances from drying experiments is proposed. A composite model of ginseng root mass transfer, based on one-dimensional treatment of diffusive and convective resistances as additive components of radial mass transfer, was developed. Mass transfer resistance was evaluated from a linear relationship between measured flux and thermodynamic driving force. Partitioning of mass transfer resistance into diffusive (core and skin) and convective (air boundary layer) resistances was done by modification of boundary conditions: (a) high (3 m/s) and low (1 m/s) air velocity; (b) skin removal. Total radial mass transfer resistance was evaluated as (146 ± 6) ∗ 106 s/m at 38°C, significantly decreasing to (48 ± 1.5) ∗ 106 s/m at 50°C. Boundary resistance was evaluated as (54 ± 5) ∗ 106 s/m at 38°C and (26 ± 3) ∗ 106 s/m at 50°C in the entire range of moisture contents. Core and skin resistances were both moisture dependent: core resistance increased from initial value of (6 ± 1) ∗ 106 s/m to (61 ± 6) ∗ 106 s/m toward the end of drying, whereas skin resistance decreased from initial value of (92 ± 5) ∗ 106 s/m to (25 ± 5) ∗ 106 s/m at the endpoint of drying. However, the sum of core and skin resistances, which represents composite diffusive resistance of intact ginseng root, was constant and independent of moisture content: (91 ± 4.6) ∗ 106 s/m at 38°C and (22 ± 1.6) ∗ 106 s/m at 50°C. The relationship between mass transfer resistance R and drying rate factor k = 1/RC was used for verification of the composite model.
ACKNOWLEDGEMENTS
I am grateful to Dr. Valerie Davidson and Dr. Ralph Brown, who helped me with valuable comments and experimental design. I especially acknowledge Dr. Larry Peterson for his help in the study and interpretation of ginseng root anatomy.