Type206: Stratified Fluid Storage Tank with Internal Heat Exchanger by R. Kubler and F. Muller As with the TRNSYS Type4, this tank is assumed to consist of NS fully-mixed equal volume segments and is discharged directly. The heat exchanger consists of NF equal volume segments each of which is coupled to a storage node according to the following rules: NF must be less than or equal to NS. The number of nodes below the heat exchanger, NDEAD, allows the user to model a dead volume in which heat only penetrates slowly by conduction. The lowermost heat exchanger node is always in contact with the lowermost 'active' storage node, i.e. with node no. NS-DEAD. Special features of the model are: - The charge flow always enters from the top of heat exchanger and flows downward. (except if NF = 1) - The load flow always enters the storage in the bottom (Node NS) and leaves the storage at the top (Node 1). - The heat exchanger fluid heat capacity is taken into account in the model, so that heat exchangers with large fluid content can be modeled accurately. There is no restriction on the heat exchanger fluid content. - The heat transfer capacity rate of the heat exchanger (UA)f,s is assumed to be constant and equally distributed over the NF nodes, the option for flow and temperature dependent (UA)f,s will be included in a future version. - No inversion layers are allowed in the storage, a mixing routine eliminates them after each time step. - The subroutine TYPE74 chooses its own optimum time step, depending on the operating conditions, which is less than or equal to the time step chosen for the simulation. Therefore the results delivered by the storage model are not sensitive to simulation time step size and the user need not bother about it as when using the other storage models TYPE4 and TYPE38. - The differential equations are solved inside the subroutine without using the TRNSYS module DIFFEQ, therefore no derivatives are specified. - The internal heater receives the heating power as input and is not equipped with a controller. During a storage test the heating power is always measured, therefore validation requires the heating power as input. A thermostat control can be simulated with TRNSYS with the help of the heater TYPE6 and the on-off controller TYPE2. The on-off controller receives the temperature from the layer in which the thermostat is placed (Output no. 10+ NT), campares it with the set value and turns the auxiliary heater on and off. The auxiliary heater supplies its power output to the auxiliary input of the storage TYPE74. The heat balance for each storage node is represented by this equation: M[s] * C[p,s] dT[s,j] -------------- * --------- = dM[s] * C[p,s] * (T[s,j+1] - T[s,j]) NS dT (UA)[f,s] + eps1 * ----------- * (T[f,k] - T[s,j]) NS d dT[s,j] + eps2 * (UA)ss * ---( ---------) dx dx (UA)[s,a] - ---------- * (T[s,j] - T[a]) NS eps1 = 1 if the storage node is in contact with the heat exchanger node eps2 = 1 if the dM[s] = 0 and dM[f] = 0 eps2 = 0 if dM[s] > 0 or dM[f] > 0 The heat exchanger equation looks similar; M[f] * C[p,f] dT[f,k] ---------------- * --------- = dM[f] * C[p,f] * (T[f,k-1] - T[f,k]) NF dT (UA)[f,s] + ---------- * (T[s,j] - T[f,k]) NF (UA)[f,a] - ---------- * (T[f,k] - T[a]) NF An important point is the difference in the definition between (UA)[f,s] as is used in TYPE74, and (UA)[f,s] as is commonly used in heat exchanger theory. (UA)[f,s] is based on the temperature difference between the exit temperature of a heat exchanger node and the corresponding storage temperature, while commonly (UA)[f,s] is based on the log-mean temperature difference. The relation between (UA)[f,s] and (UA)[f,s] is described by this equation. NF (UA)[f,s] SUMMATION( ----------- * (T[f,k] - T[s,j])) k=1 NF (T[f,i] - T[s,j1]) - (T[f,NF] - T[s,j2]) = (UA)[f,s] * ---------------------------------------- T[f,i] - T[f,j1] ln ( ------------------ ) T[f,0] - T[f,j2] where j = NS-NDEAD-NF+K j1 = NS-NDEAD-NF+1 j2 = NS-NDEAD REf: Model 4PORT for TRNSYS by R. Kubler, F. Muller July 1991 Univ. of Stuttgart FAX: 685 3242