An intentional or accidental opening in a pipeline containing a subcooled liquid at a high pressure may produce its rapid depressurization (blowdown). The liquid starts to flash when its pressure reaches the local saturation pressure and flows thereafter as a two-phase mixture. The modeling of this process plays a crucial role in the analysis of accident scenarios and in the design of controlled depressurization systems in chemical, nuclear, and offshore industries.Prediction of transfer of heat from the pipe wall to the two-phase flow during the depressurization process is a transient conjugated heat-transfer problem since the heat-transfer rate at the wall-fluid interface and local fluid conditions are directly dependent on each other and need to be simultaneously calculated. A number of approaches to the solution of this problem have been developed for a single-phase pipe flow. Approximation methods in which the thermal capacity of the pipe wall is assumed negligible were proposed by Siege1 (19601, Sucec (1975), andLi (1986). Based on the lumped capacitance approach to the transient heat conduction in the wall, Sucec (1981) and Lin (1991) obtained exact analytical and numerical solutions for a finite wall thermal capacity. Later, Lin and Kuo (1988) included the effect of the internal thermal resistance of the wall by using a one-dimensional (1-D) model of transient heat conduction in the radial direction.Much of the past work on the pipeline blowdown has concentrated on the development of models describing the hydrodynamics of the two-phase pipe flow. In these models the flow is assumed either adiabatic or isothermal (Grolmes et al., 1984;Richardson and Saville, 1991). Chen et al. (1995) formulated a model for a two-phase blowdown which takes into account forced convection heat transfer between the pipe wall and the fluid flow. However, the effects of wall thermal capacity and transient conduction are assumed negligible in their study. This approach can be used for heat transfer in flows bounded by very thin walls. The ratio of wall thickness to the internal diameter for steel pipes employed in the transport of flashing liquids reaches 0.13 (Engineering Data Book, 1972) and, therefore, a large amount of heat may be transferred to the fluid during a pipeline blowdown. Solving the conjugate heat-transfer problem for a flashing flow in a pipe is a complex problem due to difficulties associated with the modeling of forced convection in the conditions of twophase flow. The traditional approach to the solution of this problem is based on the use of empirical two-phase forced convection correlations in conjunction with a 1-D or 2-D numerical model of heat conduction in the transverse direction (Erickson and Mai, 1992). Recently, Fairuzov (1998) developed a novel approach to the description of heat transfer in long two-phase pipelines in which the effect of the thermal capacitance of the pipe wall (p,c,,,V,) is incorporated into the energy equation for the fluid flow in the form of an additional term.In this note,...