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J. Dairy Sci. 89:4475-4489
© American Dairy Science Association, 2006.

Heat Treatment of Whole Milk by the Direct Joule Effect—Experimental and Numerical Approaches to Fouling Mechanisms

L. Fillaudeau*,1, P. Winterton*, J. C. Leuliet{dagger}, J. P. Tissier{dagger}, V. Maury{dagger}, F. Semet{dagger}, P. Debreyne{dagger}, M. Berthou{ddagger} and F. Chopard§

* Institut National des Sciences Appliquées (INSA), Laboratoire de Biotechnologie–Bioprocédés, Centre National de la Recherche Scientifique (CNRS) Unité Mixte de Recherche (UMR) 5504, Institut National de la Recherche Agronomique (INRA) UMR 792-135, avenue de Rangueil, F-31077 Toulouse Cedex 4, France
{dagger} INRA–Laboratoire de Génie des Procédés et Technologie Alimentaires (LGPTA) 369, rue Jules Guesde, 59650 Villeneuve D’Ascq Cedex, France
{ddagger} EDF-R&D, Les Renardières, 77818 Moret Sur Loing Cedex, France
§ Alfa-Laval Vicarb, rue du Rif Tronchard, 38120 Fontanil-Cornillon, France

1 Corresponding author: Luc.Fillaudeau{at}insa-toulouse.fr

The development of alternative technologies such as the direct Joule effect to pasteurize and sterilize food products is of great scientific and industrial interest. Our objective was 1) to gain insight into the ability to ensure ultra-high-temperature treatment of milk and 2) to investigate the links among thermal, hydraulic, and electrical phenomena in relation to fouling in a direct Joule effect heater. The ohmic heater [OH; E{bot}v (where E is the electrical field and v is the velocity); P (power) = 15 kW] was composed of 5 flat rectangular cells [e (space between the plate and electrode) = 15 mm, w (wall) = 76 mm, and L (length of the plate in plate heat exchanger or electrode) = 246 mm]—3 active cells to ensure heating and 2 (at the extremities) for electrical insulation and the recovery of leakage currents. In the first step, the thermal performance of the OH was investigated vs. the flow regimen [50 < Re (Reynolds number) < 5,000], supplied power (0 < P < 15 kW), and electrical conductivity of fluids (0.1 < {sigma}20°C < 2 S/m) under clean conditions with model fluids. This protocol enabled a global thermal approach (thermal and electrical balance, modeling of the temperature profile of a fluid) and local analysis of the wall temperature of the electrode. An empirical correlation was established to estimate the temperature gradient, TwTb (where Tw is the wall temperature and Tb is the product temperature) under clean conditions (without fouling) and was used to define operating conditions for pure-volume and direct-resistance heating. In the second step, the ability of OH to ensure the ultra-high-temperature treatment of whole milk was investigated and compared with a plate heat exchanger. Special care was taken to investigate the heat transfer phenomena occurring over a range of temperatures from 105 to 138°C. This temperature range corresponds to the part of the process made critical by protein and mineral fouling. The objectives were 1) to demonstrate the ability of an OH to ensure heat treatment of milk, 2) to study the thermal and hydraulic performance with an increasing power and temperature difference between the inlet and outlet of the OH, 3) to define and validate a criterion to follow heat dissipation efficiency, and 4) to compare the fouling propensity with the different configurations. A heat dissipation coefficient, RhCO, was defined and validated to monitor the fouling propensity through global electrical and thermal parameters. Finally, a numerical simulation was developed to analyze heat profiles (wall, deposit, bulk). Because of an increasing Joule effect in the static deposit, the simulation showed how wall overheating would definitively cause fouling to spiral out of control.

Key Words: ohmic heating • wall overheating • fouling • whole milk







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