Module 03 : Building blocks of PINCH Technology. Lecture 07 : Hot and Cold Composite Curves and The Pinch

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Module 03 : Building blocks of PINCH Technology Lecture 07 : Hot and Cold Composite Curves and The Pinch Key words: Pinch, T H diagram, Hot utility, Cold Utility, Composite Curve, T min Pinch analysis is a methodical examination of thermally intensive processes in which all heating and cooling loads (actual or potential) are extracted as temperature/energy flow (T/H) profiles and integrated into composite curves for the whole process and/or site. The following diagrams illustrate the principle of composite curves and show how by combining the hot and cold composites the total potential for heat recovery of the plant can be quantified. This concept can be explained using a hot and a cold stream as given below: Table 3.7: Two stream problem for prediction of hot and cold utility demand Name of the stream Supply Temperature Ts, C Target Temperature Tt, C CP kw/ C H kw Hot 1 210 50 1.5 240* Cold 1 90 160 3 210 * ve sign indicates that the stream is supplying heat The above system can be pictorially shown below in Fig.3.20: Cold Stream Amount of cold utility? Temp.? Cold water Cold Utility Hot Stream 210 C? Amount of hot utility? Steam heating 16 C Hot Utility 140 Fig.3.20 Pictorial view of the problem given in Table 3.7 Figure 3.20 shows the supply and target temperature of hot 1 and cold 1 and position where hot and cold utility are to be supplied. However, it does not provide the amount of cold and hot utilities required and also the amount of internal heat exchange by the Hot 1 and cold 1 streams. Due to incomplete information the exit temperatures of streams from the heat exchanger could not be computed.

T, C 210 C HU= 45 kw HU= 30 kw 160 C a b T min = 10 C 0 50 100 150 200 250 300 CU= 60 kw CU= 75 kw Fig. 3.21 Prediction of hot and cold utility demands as a function of T min From Fig.3.21 it can be seen that when cold 1 is shifted horizontally towards Hot 1 stream so that it touches the hot 1 stream(position a ) the available T between hot and cold stream at one end becomes zero. This is possible as the reference enthalpy for a cold stream can be changed independently from the reference enthalpy for the hot streams. The point at which the cold stream meets the hot stream is called Pinch Point. However, in most of the cases Pinch Point is not a point but two points called hot pinch point and cold pinch point and are expressed in terms of temperatures. At this point the hot utility (HU) and cold utility(cu) demands are minimum and are equal to 30kW and 60kW respectively. The heat exchange between hot 1 and cold 1 becomes maximum and is equal to 180 kw. Further the total heat exchange including HU and CU becomes 270 kw. However this case is practically infeasible as at T=0 no heat transfer can take place and area required for heat transfer becomes infinite. So this marks one extreme condition. To make the heat transfer feasible the cold 1 stream is shifted parallel to a new position b where the vertical distance between its supply temperature end and line representing Hot 1 stream becomes 10 C. This distance is called T min. The value and concept of of T min is important as it fixes the relative position of hot and cold stream ( or Hot composite and cold composite). As supply end of cold 1 stream is kept at T min = 10 C from Hot 1 stream the HU and CU demands grow to 45 kw and 75 kw and the internal heat exchange between Hot 1 and Cold 1 becomes 165 kw. The total heat exchange including CU and HU becomes 285 kw. For this case the hot pinch is at 100 C and cold pinch is at the difference being equal to T min.

Thus it can be concluded that HU, CU and amount of internal heat exchange is a function of T min. After the above analysis now one is in a position of filling the unknown information of Fig.3.20 as given in Fig.3.22. Amount of cold utility 75kW 100 C Cold water Cold Utility For T min = 10 C Amount of hot utility 45kW Cold Stream Hot Stream 210 C 145 C Steam heating 16 C Hot Utility 160 Fig.3.22 Pictorial view of the solved problem given in Table 3 After dealing with a two stream problem a comparatively difficult problem as given by stream data of Table 3.8 is considered for prediction of energy target based on Hot and Cold composite curves and T min equal to 10 C. These curves are shown in Fig.3.23. Table 3.8: Four stream problem for load integration and utility prediction for T min equal to 10 C. Name of the stream Supply Temperature Target Temperature CP Ts, C Tt, C kw/ C Hot 1 140 50 2 180 Hot 2 90 40 6 300 Cold 1 30 150 2 240 Cold 2 70 125 3 165 H kw T, C 140 C HOT COMPOSITE CURVE 40 C H= 480 (a)

T, C 1 125 C COLD COMPOSITE CURVE 70 C H=405 Fig.3.23 (a) Hot composite curve, (b) Cold composite curve for problem given in Table 3.8 (b) Combined Hot and Cold Composite curves Once Hot and cold composite curves are created these can be put together to extract useful information regarding energy change and external utility demand. T, C Internal Heat Exchange External Hot utility Q HOT, MIN 1 140 C 125 C a b c Hot Pinch Cold Pinch 80 C 70 C T min = 10 C 40 C External Cold utility Q COLD, MIN Fig.3.24 Determination of energy targets utilizing Hot and Cold composite curves

In Fig.3.24 the hot and cold composites are plotted on the same T H axes keeping intact the temperature of both hot and cold composite curves. Hot composite curve contains temperature level of 140 C,, and 40 C( marked by solid lines) and the temperature levels for cold composite curves are 1, 125 C,70 C and ( shown by dotted lines except as it matches with axis). The cold composite curve is then moved from position c (original position) to position a where the shortest vertical distance between hot and cold composite curves is 10 C which is the T min in this case. Due to the kinked nature of composite curves the point of T min can occur anywhere in the region of internal heat exchange and not just at one end of any composite curve. The temperature enthalpy values associated with any composite stream can t be changed, however, the relative position of composite streams can be changed by moving them horizontally( parallel to H axis) relative to reach other. This is possible as the reference enthalpy for the cold composite stream can be changed independently from the reference enthalpy for the hot composite streams. For a given value of T min the cold and hot utilities computed are the minimum required values to keep the system in thermal balance. Specifying the hot utility or cold utility or T min fixes the relative position of the two composite curves. The relative position of the two curves is a degree of freedom available to process designer which can be changed by moving these horizontally relative to each other. The shortest vertical distance between two composite curves is called T min. In general, T min occurs at only one point which is called the Pinch point. This implies that except at or T min in all other places the vertical distance between two composite curves ( which is in fact T) will be greater than or T min. Due to the minimum driving force available at T min the design is most constricted here. Further the heat exchanger matches at or T min or near it will have large heat transfer area in comparison to heat exchanger matches which are away from it. When the curves touch each other there is no driving force for heat transfer at one point of the process, which would require infinite heat transfer area and hence infinite capital cost. It should be noted that the composite curves are made up of many streams. The T min at a certain point between hot and cold composite curves indicate that the all the hot streams present at this point will have a temperature difference of T min ( at least at one end of it) with all the cold streams present at that point. So it is possible to design a HEN which will operate the heat exchangers at Pinch Point with T values equal to T min. This HEN will demand minimum utility as computed by bringing hot and cold composite curves to a minimum vertical distance of T min.

T, C Internal Heat Exchange External Hot utility Q HOT, MIN 1 140 C Hot Pinch Cold Pinch 125 C 80 C 70 C 40 C Hot Composite curve Pinch Points T min = 10 C Cold Composite curve External Cold utility Q COLD, MIN Source Section Sink Section Below the Pinch Above the Pinch Fig.3.25 Shows both composite curves put together for problem given in Table 3.8 From Fig.3.25 it can be seen that hot utility demand is 175 kw, cold utility demand is 250 kw and internal heat exchange is 230 kw. This is for T min equal to 10 C. The hot pinch point is at and cold pinch point is at 80 C. Main points regarding combined Hot and cold composite curves are: 1. To consider heat recovery from hot stream to cold streams, it is necessary that the complete hot composite curve must be above the cold composite curve for natural heat transfer to take place. 2. The relative position of Hot and cold composite curves can be fixed by fixing Hot utility or Cold utility or T min. 3. The over lapping between hot and cold composite curves determine the maximum extent of internal heat exchange between hot and cold streams. 4. The over shoot of cold composite curve (beyond hot composite curve) indicates the minimum amount of external hot utility required for the process. 5. Similarly the over shoot of hot composite curve (beyond cold composite curve) determines the minimum external cold utility demand. 6. The Hot and cold utility demands and the amount of internal heat exchange is a function of T min. 7. The T min is defined at pinch point. At this place the vertical distance between two composite curves are minimum and thus it is called T min. The vertical distance between

cold and hot composite curves at any place indicates the driving force T which exists at that place. The minimum driving force exists at T min. 8. Pinch divides the complete heat integration problem in two parts Above pinch region (upper pinch) and below pinch region (lower pinch). This is so as in the case of a Maximum Energy recovery design (MER) for a certain value of T min no heat transfer takes place across pinch point. Though physically the heat integration problem appears undivided in terms of the resulting HEN, as far as heat transfer is concerned it is divided in two parts. 9. The Upper pinch area is a heat sink as heat is supplied to this area through external hot utility. The lower pinch area works as a heat source as it transfers heat to a cold utility. 10. The combined hot and cold utility curve helps in plant layout as it indicates which hot stream should be close to which cold stream for minimum piping. It also indicates where the Boiler and Cooling tower should be located which respect to streams. 11. As upper pinch region is a net sink no cold utility should be used here. If a cold utility of amount say X cold is used in this region then the hot utility demand has to be increased to Q Hmin + X cold to satisfy the heat balance of this region. Thus it will increase the hot utility demand. At the same time total consumption of cold utility will also increase to Q Cmin + X cold. Thus both cold and hot utilities will increase from their minimum value by an amount X cold. So the penalty will be double in terms of the increased cost of utility as well as heat transfer area required to transfer the heat associated with increased amount of utility. 12. Similarly as lower pinch area is a net heat source and hot utility should not be used here. If a hot utility of amount say X hot is used in this region then the cold utility demand has to be increased to Q Cmin + X hot to satisfy the heat balance of this region. Thus it will increase the total cold utility demand. At the same time total consumption of hot utility will also increase to Q Hmin + X hot. Thus both cold and hot utilities will increase from their minimum value by an amount X hot. So the penalty will be double in terms of the increased cost of utility as well as heat transfer area required to transfer the heat associated with extra amount of utility. References 1. Linnhoff March, Introduction to Pinch Technology Targeting House, Gadbrook Park, Northwich, Cheshire, CW9 7UZ, England 2. Chemical Process Design and Integration, Robin Smith, John Wiley & Sons Ltd. 3. Ian C Kemp, Pinch Analysis and process integration, a user guide on process integration for effective use of energy, IChem E, Elsevier Limited, 2007.