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Title: Tier II: Case Studies


1
(No Transcript)
2
Tier II Case Studies
  • Section 2
  • Heat Exchange Network Optimization by Thermal
    Pinch Analysis

3
Optimization Problems
  • There are many different types of optimization
    problems
  • It is important to recognize that an optimization
    problem exists even if it does not immediately or
    easily lend itself to one of the previously
    described analytical methods of optimization
  • Sometimes an alternative method that is more case
    specific must be used

4
Optimization Problems
  • A common example of one of these problems is the
    optimization of a heat exchange network
  • Without knowing what the maximum possible network
    integration is, and the minimum possible heating
    and cooling utilities required, it can be very
    difficult to design an optimized heat exchange
    network

5
Optimization of Utility Use in a Heat Exchange
Network
  • Heating and cooling utilities consumption can be
    treated as an optimization problem
  • The goal is to minimize the amount of heating and
    cooling utilities being used by optimizing the
    heat exchange network
  • A different method will be used for this type of
    optimization than what was seen previously

6
Constraints
  • Total heating (QH) and total cooling (QC) used
    will still need to be minimized according to a
    set of constraints
  • These constraints are
  • The target temperature of individual streams
  • The minimum approach temperature in a heat
    exchanger

7
Constraints
  • Objective function
  • Minimize QH QC
  • Constraints
  • T2i ai , T1i bi
  • t1i ci , t2i di
  • DTmin k

8
Minimum Approach Temperature
T1 hot out T2 hot in t1 cold in t2 cold
out
9
Minimum Approach Temperature
  • To get the outlet temperature of one stream
    closer to the inlet temperature of the other
    stream, exchanger area must be increased,
    increasing capital cost
  • Decreased exchanger area means decreased capital
    cost, but increased utilities cost to make up for
    lost heat exchange capacity

10
Using Minimum Approach Temperature to Tradeoff
Capital vs. Operating Costs
  • This graph demonstrates the tradeoff between
    capital and operating costs a decrease in one
    is met with an increase in the other

11
Minimum Approach Temperature
  • The optimum exchanger size exists where the total
    annualized cost is minimized
  • This typically will correspond to a minimum
    approach temperature, DTmin of about 10oC
  • This DTmin 10oC is a rule of thumb it can
    change depending on the fluid service and the
    type of heat exchanger employed

12
Minimum Approach Temperature
  • Thermal Equilibrium
  • T t
  • Practical Feasibility
  • T t DTmin
  • This must be included in the coming analysis

13
Graphical Method Thermal Pinch Analysis
  • To optimize a heat exchange network, an example
    of the graphical method to determine the thermal
    pinch point will first be examined
  • The same example will then be solved using the
    algebraic method for comparison

14
Stream Data
  • Using the stream supply and target temperatures,
    the enthalpy change of each stream must be
    calculated
  • Enthalpy change
  • DH FiCpi(T2i T1i) HHi
  • FiCpi(t2i t1i) HCi
  • FiCpi flow rate x specific heat (kW/K)

15
Stream Data
Hot Stream FiCpi Supply (oC) Target (oC) Enthalpy Change
  (kW/oC) T2i T1i HHi, (kW)
H1 400 340 260 32000
H2 350 400 360 14000
H3 300 450 380 21000

Cold Stream FiCpi Supply (oC) Target (oC) Enthalpy Change
  (kW/oC) t1i t2i HCi, (kW)
C1 250 240 290 12500
C2 300 300 400 30000
C3 450 350 400 22500
16
Stream Data
  • Stream data is then plotted as a series of
    straight line segments in order of ascending
    temperature
  • Each consecutive segment begins at the enthalpy
    level where the previous segment finished
  • A hot stream is any that must be cooled, while
    a cold stream is any that must be heated,
    regardless of supply temperature

17
Hot Streams
18
Cold Streams
19
Composite Stream Curves
  • Next the composite curves of the hot and cold
    streams must be constructed
  • These composite curves represent the total amount
    of heat to be removed from the hot streams and
    the total amount of heat that must be added to
    the cold streams to reach the target stream
    temperatures

20
Hot Composite Stream Construction
H3
H2
H1
T11
T21
T12
T22
T13
T23
21
Hot Composite Stream Construction
Hot composite stream
22
Cold Composite Stream Construction
C3
C2
C1
t13
t22
t21
t11
t12
t23
23
Cold Composite Stream Construction
Cold composite stream
24
Optimizing the Heat Exchange Network
  • The cold composite stream must now be
    superimposed over the hot composite stream to
    perform the thermal pinch analysis
  • This will give the minimum amount of utilities
    required to reach the target states
  • Note how the temperature axis is shifted for the
    cold composite stream to account for the minimum
    approach temperature

25
No Heat Integration
Total hot utility required
Cold composite stream
QH,max 65,000 kW
Total cold utility required
Hot composite stream
QC,max 67,000 kW
QC QH 132,000 kW
26
No Heat Integration
  • With no heat integration, the amount of energy
    required to reach the target state is maximized
  • In this case the total amounts of energy required
    are
  • Cooling utility, QC 67,000 kW
  • Heating utility, QH 65,000 kW
  • Total utilities QC QH 132,000 kW
  • Clearly there is room for optimization

27
Partial Heat Integration
  • By moving the cold composite stream down a bit, a
    partially integrated heat exchange network is
    graphically represented
  • Some heat is transferred from hot streams to cold
    streams to approach the temperature targets

28
Partial Heat Integration
Cold composite stream
Hot composite stream
QC QH 102,000 kW
29
Partial Heat Integration
  • This heat exchange network is only partially
    optimized and already utility consumption is
    reduced by 30,000 kW
  • The utilities required are
  • Cooling utility, QC 52,000 kW
  • Heating utility, QH 50,000 kW
  • Total utilities QC QH 102,000 kW
  • Clearly further integration can provide
    significant energy savings

30
Optimized Heat Integration
  • To determine the optimized heat exchange network,
    the thermal pinch point must be found
  • This is accomplished by moving the cold composite
    stream down just until one point on the line
    meets a point on the hot composite line
  • This point is the thermal pinch point

31
Optimized Heat Integration
QH,min 8,500 kW
Cold composite stream
Integrated heat exchange 56,500 kW
Pinch point
Hot composite stream
QC,min 10,500 kW
240
QC QH 19,000 kW
32
Optimized Heat Integration
  • The heat exchange network is now fully optimized
  • Total required utilities are minimized
  • Minimum cooling utility, QC,min 10,500 kW
  • Minimum heating utility, QH,min 8,500 kW
  • Minimum total utilities QC QH 19,000 kW
  • No heat is passed through the pinch point

33
Passing Heat through the Pinch Point
  • To have an optimized heat exchange network, it is
    critical that no heat is passed through the
    thermal pinch point
  • By passing an amount of heat, a, through the
    pinch point, an energy penalty of 2a is added to
    the total utilities requirement
  • It is very important to maximize integration in a
    heat exchange network

34
Passing Heat Through the Pinch Point
QH QC QH,min QC,min 2a
35
Crossing the Pinch Point
  • It would appear that extra energy can be saved by
    lowering the cold composite stream line further
  • This does not work however because it creates a
    thermodynamically infeasible region
  • For this to work, heat would have to flow from
    the cooled hot streams to the heated cold streams
    - from a cold source to a hot source

36
Crossing the Pinch Point
Cold composite stream
Pinch point
Hot composite stream
Infeasible region
37
Disregarding DTmin
  • Another tempting error is to disregard the
    minimum approach temperature
  • By disregarding a minimum approach temperature,
    the absolute minimum thermodynamically possible
    utility requirements are obtained
  • Although this is thermodynamically possible, it
    is not practically feasible as it would require
    an infinitely large heat exchanger area
  • This would obviously cost far more than the
    relatively small energy savings are worth

38
Disregarding DTmin
QH,min thermo.
QC,min thermo.
240
39
Algebraic Method
  • This same problem will now be solved using the
    algebraic method
  • This will involve producing a temperature
    interval diagram, tables of exchangeable heat
    loads, and cascade diagrams

40
Stream Data
From before
Hot Stream FiCpi Supply (oC) Target (oC)
  (kW/oC) T2i T1i
H1 400 340 260
H2 350 400 360
H3 300 450 380

Cold Stream FiCpi Supply (oC) Target (oC)
  (kW/oC) t1i t2i
C1 250 240 290
C2 300 300 400
C3 450 350 400
41
Temperature Interval Diagram
  • The first step is to construct the temperature
    interval diagram
  • This diagram shows the starting and finishing
    temperatures of each stream
  • An interval begins at a streams starting or
    finishing temperature, and it ends where it
    encounters the next beginning or finishing
    temperature of a stream
  • Draw horizontal lines across the table at each
    arrows head and tail, with the intervals lying
    between these lines
  • Note how the cold stream temperature scale is
    staggered by 10 degrees

42
Temperature Interval Diagram
43
Table of Exchangeable Heat Loads
  • The next step is to construct tables of
    exchangeable heat loads for the hot and cold
    streams
  • These tables show the amount of energy that must
    be added or removed from a stream over a
    particular interval
  • These energy values are calculated as
  • DHj,i FCpjDTi, where DTi is the positive
    temperature difference across the interval, and j
    denotes the stream number

44
Table of Exchangeable Heat Loads
  • For the hot streams,

45
Table of Exchangeable Heat Loads
  • For the cold streams,

46
Cascade Diagrams
  • Using the information from the heat load tables,
    the cascade diagrams can now be constructed
  • These diagrams will be used to determine the
    pinch point and the minimum heating and cooling
    utilities required

47
Cascade Diagram
  • First, the cascade diagram is drawn as it appears
    at right, with one box for each interval that
    appeared in the temperature interval diagram

48
Cascade Diagram
  • Next, the total values from the exchangeable heat
    load tables are added to the cascade diagram
  • Hot stream loads enter on the left, cold stream
    loads exit on the right

49
Cascade Diagram
0
  • Now, by subtracting an intervals cold load from
    the hot load, and adding the resulting value to
    the residual from the previous stage we get the
    residual value for the subsequent stage
  • ri HHi HCi ri-1

12000
7500
5500
-2500
-8500
-5500
-1500
4500
1) 12000 0 0 12000
2) 3000 7500 12000 7500
3) 13000 15000 7500 5500
5) 0 6000 -2500 -8500
6) 12000 9000 8500 -5500
8) 16000 10000 1500 4500
7) 4000 0 5500 -1500
9) 0 2500 4500 2000
4) 7000 15000 5500 -2500
2000
50
Thermal Pinch Point
  • The thermal pinch point occurs at the largest
    negative number
  • The absolute value of this number is now added in
    at the top to cascade through

51
Revised Cascade Diagram
8500
8500
8500
8500
8500
8500
8500
8500
8500
8500
52
Revised Cascade Diagram
Qmin,heating
  • We now have the final revised cascade diagram
  • It can be seen that by adding additional energy
    at the top, it will cascade through and also be
    present at the bottom

Pinch Point
QH QC QH,min QC,min 2a !
Qmin,cooling
53
Optimized Heat Integration
  • The heat exchange network is now fully optimized
  • Total required utilities are minimized
  • Minimum cooling utility, QC,min 10,500 kW
  • Minimum heating utility, QH,min 8,500 kW
  • Minimum total utilities QC QH 19,000 kW
  • As expected, these values are the same as
    obtained by using the graphing method

54
Design Considerations
  • Some design rules to optimize utility
    consumption
  • Do not pass heat through the pinch point
  • Do not use cooling utilities at temperatures
    above the pinch point
  • Do not use heating utilities at temperatures
    below the pinch point

55
Constructing the Heat Exchange Network
  • Now that the pinch analysis has been performed,
    the heat exchange network can be constructed
  • It is a good idea to perform the pinch analysis
    first because it sets the performance goal of an
    optimized heat exchange network
  • There is no quick method of reliably determining
    the minimum number of heat exchangers, but the
    following method should help to construct the
    network

56
Constructing the Heat Exchange Network
  • With QC,min and QH,min known, construct a plot
    similar to the temperature interval diagram,
    except instead of arrows, use boxes that have a
    width representing FCp
  • The area of these boxes corresponds to the heat
    exchanged by the stream
  • Draw a horizontal line across at the pinch point
    remember, no heat is to be passed across this
    point

57
Constructing the Heat Exchange Network
58
Constructing the Heat Exchange Network
  • Now, add QC,min to the lowest point on the
    coldest hot stream and determine the resulting T1
    and T2 for this exchange. Note that T1, T2, t1,
    and t2 now do not necessarily correspond to the
    same values as used earlier and are different for
    each exchanger
  • QC,min FCp(T2 T1)
  • Do the same with QH,min, adding it to the highest
    point on the hottest cold stream
  • QH,min FCp(t2 t1)

59
Constructing the Heat Exchange Network
60
Constructing the Heat Exchange Network
  • Now, working out from the pinch point, match up
    streams, remembering not to transfer heat across
    the pinch point and keeping DTmin in mind
  • For each matched stream, determine the
    temperatures that exist for the inlet and outlet
    of the heat exchanger
  • Qex FCp(T2 T1) FCp(t2 t1)
  • Having the table of stream data including
    enthalpy change on hand may be helpful for
    determining the best way to match a stream

61
Matched Streams
62
Heat Exchangers
  • 4 heat exchangers, plus a heater and a cooler are
    needed to meet the optimum heat exchange
    requirements of this system

63
Conclusion
  • There is no quick method that is guaranteed to
    give the minimum number of heat exchangers
    required every time
  • However, by first performing a thermal pinch
    analysis to determine the maximum heat exchange
    possibilities, designing an optimum network
    configuration is made a lot easier

64
References
  • Dr. El-Halwagi lecture notes
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