Summary for TEP 4215 E&P/PI
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Transcript of Summary for TEP 4215 E&P/PI
Summary forTEP 4215
E&P/PI
T. Gundersen
• Reactor System (R) Endothermic vs. Exothermic Reactions Equilibrium vs. Kinetics Temperature Dependence of Equilibrium
Constants and Reaction Rates (Arrhenius) Reactors play a key Role in the Thermal and the
Mechanical Energy System of a Plant (or Site) Correct Integration of Reactors
Sum 1
Process, Energy and System
Summary of Process Integration
R S H U
Summary forTEP 4215
E&P/PI
T. Gundersen
• Reactor / Separator Interface (R/S) Focus of the Discussion was based on the
Definition and Use of the following Terms: Degree of Conversion (Extent of Reaction) Selectivity Yield (Reactor and Process) Recycle Rate
Sum 2
Process, Energy and System
Summary of Process Integration
R S H U
YR = X · S
YP = X · S · (1 + W)R S
FF
RR
P
PX
RXRF
BP
Summary forTEP 4215
E&P/PI
T. Gundersen
• Separation System (S) Economical Trade-offs in Distillation Columns
Operating Cost vs. Investment Cost Number of Stages, Reflux and Pressure
Combinatorial Issues & Heuristic Rules related to the Sequence of Distillation Columns
Heat Integration Opportunities between Columns (Condenser / Reboiler)
Briefly about Evaporators Multi-effect, Forward/Backward Feed, BPR
Sum 3
Process, Energy and System
Summary of Process Integration
R S H U
T. Gundersen
Sequence of Distillation Columns
Sum 4
Separation Systems
Process, Energy and System
Problem Definition by Thompson and King, AIChE Jl, 1972:
”Given a mixture of N chemical components that is to be separated into N pure component products by using a selection of M separation methods”
Seq
( 1)Alt Seq
2 ( 1) !Number of Sequences
! ( 1)!
Number of Alternatives N
NN
N N
N N M
T. Gundersen
Sequence ofColumns
Sum 5
Separation Systems
Process, Energy and System
ABCD
ABCD
ABCD
ABCD
BCD
BCD
ABC
ABC
CD
BC
CD
BC
AB
AB
2 comps. 1 sequence
3 comps. 2 sequences
4 comps. 2x(1+3 comps.) + 1x(2+2 comps.) 2x2 + 1 = 5 sequences
5 comps. 2x(1+4 comps.) + 2x(2+3 comps.) 2x5 + 2x2 = 14 sequences
6 comps. 2x(1+5 comps.) + 2x(2+4 comps.) + 1x(3+3 comps.) 2x14 + 2x5 + 2x2 = 42 sequences
T. Gundersen
Sequence of Distillation ColumnsSelected Heuristic Rules
Sum 6
Separation Systems
Process, Energy and System
H1: Favor Separation of the most Volatile ComponentH2: Favor near-Equimolar SeparationH3: Favor Separation of the most Plentiful ComponentH4: Favor Simple Separations<< H5: Delay Separation of Sharp Splits >>
Heuristics cause Conflicts, some can be Quantified, others just ”cast a vote”, their
main use is to Eliminate Sequences !!
T. Gundersen
Example – Distillation Sequence
Separation Systems
Process, Energy and System
Comp. Name Mole Frac. α=Ki/Kj ”CES”
A Propane 0.052.00 5.26
B i-Butane 0.151.33 8.25
C n-Butane 0.252.40 114.50
D i-Pentane 0.201.25 13.46
E n-Pentane 0.35
Nadgir & Liu, AIChE Journal, 1983:
f = min (D/B, B/D) Δ = (α – 1)100 CES = f α
Sum 7
Summary forTEP 4215
E&P/PI
T. Gundersen
• Heat Recovery System (H) Targets for best Performance
Minimum Energy from the Heat Cascade Minimum Energy Cost with Multiple Utilities from
the Grand Composite Curve Fewest Number of Units from the (N – 1) Rule Minimum Area from Spaghetti Design (“Bath”) Total Annual Cost vs. ΔTmin
3-Way Trade-off (Area, Energy and Units)
Sum 8
Process, Energy and System
Summary of Process Integration
R S H U
T. Gundersen Sum 9
Process, Energy and System
Summary of Process Integration
Heat Cascade as Algorithm/Procedure (1)(0) Given Set of Hot Stream Temperatures: TH , i = 1,nH , Set of Cold Stream
Temperatures: TC , j = 1,nC , and Set of mCps, i = 1,nH , j = 1,nC
(1) Calculate Shadow Temperatures from Hot Streams: THS , TH,S=TH−ΔTmin
(2) Calculate Shadow Temperatures from Cold Streams: TCS , TC,S=TC+ΔTmin
(3) Obtain Total Set of Hot Stream Temperatures, THT, by merging and sorting TH and TCS Notice that dim (THT) = nH + nC
(4) Obtain Total Set of Cold Stream Temperatures, TCT, by merging and sorting TC and THS Notice that dim (TCT) = nC + nH
(5) Remove possible Duplicates in THT and TCT. The number of Temperature Intervals is then K = dim (THT) − 1
(6) Temperature Intervals are now obtained by using one Temperature from THT and one from TCT starting at the highest Temperatures
(7) Identify Heat Flows from all the Hot Streams to the respective Temperature Intervals based on mCp values and Interval Temperatures
T. Gundersen Sum 10
Process, Energy and System
Summary of Process Integration
Heat Cascade as Algorithm/Procedure (2)(8) Identify Heat Flows from the respective Temperature Intervals to all the
Cold Streams based on mCp values and Interval Temperatures
(9) Calculate the Enthalpy (Heat) Balance (Surplus or Deficit) for each Temperature Interval
(10) Cascade Heat from the first Interval to the second, and from the second to the third Interval. Continue to the end of the Cascade
(11) If all Residuals (i.e. Heat from one Interval to the next) are non-negative (Rk ≥ 0), then no External Heating is required, QH,min = 0, and Minimum External Cooling is obtained as the Residual from the last Interval, i.e. QC,min = RK
(12) If at least one Residual is negative, then Minimum External Heating and Cooling are: QH,min = − min ( Rk) , k = 1,K-1 , QC,min = RK + QH,min
(13) The Process Pinch is the Interval Temperature with the most negative Residual which has zero heat flow after adding Minimum External Heating to the Cascade
T. Gundersen Sum 11
Process, Energy and System
Summary of Process Integration
Example: Stream Data from Assignment 3
Stream Ts(°C) Tt (°C) mCp (kW/°C) ΔH (kW)
H1 170 60 3.0 330 H2 150 30 1.5 180 C1 20 135 2.0 230 C2 80 140 4.0 240
ΔTmin = 10°C
THT = 170, 150, 145, 90, 60, 30TCT = 160, 140, 135, 80, 50, 20 K = 6 – 1 = 5
T. Gundersen Sum 12
Process, Energy and System
Summary of Process Integration
Example: Stream Data from Assignment 3
90°C 80°C
+ 2.5
- 82.5
+ 75
- 15
C1
C2
H2
H160 kW
15 kW
170°C 160°C
150°C 140°C
145°C 135°C
60°C 50°C
30°C 20°C
7.5 kW
165 kW
82.5 kW
45 kW
90 kW
45 kW
20 kW
220 kW
110 kW
60 kW
60 kW
+ 60
R1=60
R4=55
R5=40
R2=62.5
R3=−20
T. Gundersen
Process, Energy and System
Investment Cost
WS-8 cont.Vertical Design:
2 − 3 and 1 − 4
Criss-Cross Design:2 − 4 and 1 − 3
200
250
300
350
0 500 1000
1
2
3
4
T(°C)
Q(kW)
2
2
500 500 1616.4 m0.00909 68.05 0.00909 68.05
500 500 1000 250 1250 m0.005 100 0.05 40
vertical
criss cross
A
A
Explanation: Optimal Distribution of (UΔT) - not only ΔT
Sum 13
Summary forTEP 4215
E&P/PI
T. Gundersen
• Heat Recovery System (H) Design of Network using PDM
Decomposition at Pinch (Process and Utility Pinch) Start the Design at the Pinch Pinch Exchangers and Requirements
mCp Rules: mCpout ≥ mCpin
Population: nout ≥ nin
Focus on ΔT, not ΔH Tick-off Rule Check Design against Targets !!
Sum 14
Process, Energy and System
Summary of Process Integration
R S H U
Summary forTEP 4215
E&P/PI
T. Gundersen
• Heat Recovery System (H) Optimization of Heat Exchanger Networks
Stream Splitting (start with: α/β = mCp1/mCp2) Heat Load Loops and Paths
The HEN Design Process as a “Flow Diagram” Retrofit Design of Heat Exchanger Networks
Targeting for good value of HRAT XP Analysis (QP = QPP + QPH + QPC) Shifting to reduce XP Heat Transfer UA Analysis (existing and new) followed by Loops
and Paths for maximum Reuse of existing Units
Sum 15
Process, Energy and System
Summary of Process Integration
R S H U
T. Gundersen Sum 16
Process, Energy and System
Summary of Process Integration
H1
C3
I CaQI = 3500 kW QCa = 4300 kW
180ºC
130ºC
60ºC
50ºC
H2
C2 C1
CbIIIII
H 105ºC
190ºC
70ºC
40ºC100ºC
200ºC
QH = 3600 kW
QCb = 300 kW
QIII = 1300 kW
QII = 3600 kW
Exam 2 June 2008 – Retrofit (60%)
mCp = 60 kW/°C
mCp = 50 kW/°C
mCp = 40 kW/°C
mCp = 20 kW/°C
mCp = 80 kW/°C
ΔTmin = 10°C
T. Gundersen Sum 17
Process, Energy and System
Summary of Process Integration
Exam 2008
50°C 40°C
200
+ 1200
CW
ST
C2
C3
H1
H2800 kW
2800 kW
200°C 190°C
180°C 170°C
110°C 100°C4200 kW
5600 kW
2000 kW
1600 kW 800
QH
R1
QC
R2
1600 kW
1500 kW
2400 kW
+ 800
70°C 60°CR3
1200 kWC1
100 kW
800 kW
400 kW
50°C 40°C
200
+ 1200
CWCW
ST
C2C2
C3C3
H1H1
H2H2800 kW
2800 kW
200°C 190°C
180°C 170°C
110°C 100°C4200 kW
5600 kW
2000 kW
1600 kW 800
QH
R1
QC
R2
1600 kW
1500 kW
2400 kW
+ 800
70°C 60°CR3
1200 kWC1C1
100 kW
800 kW
400 kWH,exist
C,exist
H,min
C,min
H C
3600 kW
4600 kW
1000 kW
2000 kW
2600 kW
Q
Q
Q
Q
Q Q
Simplified Cascade withSupply Temperatures only
T. Gundersen Sum 18
Process, Energy and System
Summary of Process Integration
Exam 2008 Cross-Pinch Analysis
H1
H2 Cb
C1
180°
77.5°200°
105°
130°
121.67°
60°
40°
70°
50°
mCp(kW/°C)
[60]
[40]
[20]
[50]I C3
II
I
III
110°
100°
190°100° [80]II C2
Ca
H
III
145°
110°
3500
36003600
1300
4300
300
XP 50 (100 60) 60 (121.67 110) 20 (105 100) 2000 700 100 2600 kWQ
T. Gundersen Sum 19
Process, Energy and System
Summary of Process Integration
Exam 2008
y can be found by ΔTmin requirements y = 1500 kW
Next: What about Investments ??
H1180°
200°
130°
121.67°
60°
50°
mCp(kW/°C)
[60]
[50]I C3
I
190°145°
[80]IV C2
Ca
H
3500
0 + y3600-y
4300-y
IV
“Shifting”
TH1
T. Gundersen Sum 20
Process, Energy and System
Summary of Process Integration
Exam 2008
Next: UA Analysis for maximumReuse of existing Exchangers
H1
H2 Cb
C1
180°
77.5°200°
105°
130°
96.67°
60°
40°
70°
50°
mCp(kW/°C)
[60]
[40]
[20]
[50]I C3
II
I
III
190° 100°[80]II C2
Ca
H
III
145°
110°
3500
36002100
1300
2800
300
IV
IV
1500
155°
163.75°
Summary forTEP 4215
PI
T. Gundersen
• Separation/Heat Recovery Interface (S/H) Columns integrated above/below Pinch
Condenser above, Reboiler below Which Pinch – Columns often create Pinch
Extended Grand Composite Curve (Andrecovich) Distinguish Columns from “Background” Process
Evaporators and Heat Integration The Tool is again the Grand Composite Curve Play with Pressure and the Number of Effects
Sum 21
Process, Energy and System
Summary of Process Integration
R S H U
Summary forTEP 4215
PI
T. Gundersen
• Heat Recovery / Utility Interface (H/U) Correct Integration of Heat Pumps (open/closed) Correct Integration of Turbines (back pressure
or extraction vs. condensing turbines) Co-production of Heat & Power (cogeneration) The quantitative Tool with Information about
Load (heat duty) and Level (temperature) is: The Grand Composite Curve Modified Temperatures are important !!
Sum 22
Process, Energy and System
Summary of Process Integration
R S H U
Summary forTEP 4215
PI
T. Gundersen
• Utility System (U) Not treated in much Detail in this Course Topics could (or should?) have been:
Design of Steam Systems (turbines, boilers, deaerators, etc.)
Design of fired Heaters (Furnaces) with optimal preheat of Combustion Air
Design of Refrigeration Cycles including Integration with the Process (“economizers”)
Etc., etc.
Sum 23
Process, Energy and System
Summary of Process Integration
R S H U
Summary forTEP 4215
PI
T. Gundersen
• Other Topics Optimization: Only Demo with Examples from
Heat Recovery using Math Programming Forbidden Matches & Extended Cascade is relevant
Operational Aspects (especially related to Flexibility and Controllability)
The Importance of Topology (Structure) Extensions of the Pinch Principle
Heat Pinch, Mass Pinch, Water Pinch and Hydrogen Pinch (whenever an “amount” has a “quality”)
Sum 24
Process, Energy and System
Summary of Process Integration
R S H U
More on the Grand Composite Curve
Reactor
Feed
Product
DistillationColumn
Compressor
50°
210°
160°
210°
130°
220°
160°
270°
60°Reboiler
Condenser
T. Gundersen
Heat Integration − Introduction
Process, Energy and System
Extra 01
H1
H2
C1
C2
Grand CompositeCurve is based
on the HeatCascade
T. Gundersen Extra 02
Process, Energy and System
Heat Integration − Targeting
270ºC - - - - - - - 250ºC
230ºC - - - - - - - 210ºC
220ºC - - - - - - - 200ºC
180ºC - - - - - - - 160ºC
160ºC - - - - - - - 140ºC
70ºC - - - - - - - - 50ºC
H1
H2
CW
C1
C2
ST
720 kW
180 kW
720 kW
880 kW
440 kW
1980 kW
500 kW
200 kW
800 kW
1800 kW
+ 720
- 520
- 1200
2000 kW
400 kW
+ 180
+ 220
+ 400
60ºC - - - - - - - - 40ºC
360 kW
220 kW
ΔTmin = 20°C
The necessarydata are modified
Temperatures and thecorresponding Heat Flows
T6’ = 50 QC,min = 800
CW
ST
+ 720
- 520
- 1200
+ 180
+ 220
+ 400
T0’ = 260 QH,min = 1000
T1’ = 220 R1 = 1720
T2’ = 210 R2 = 1200
T3’ = 170 R3 = 0
T4’ = 150 R4 = 400
T5’ = 60 R5 = 580
Grand Composite Curve(or Heat Surplus
Diagram)
T. Gundersen Extra 03
Process, Energy and System
Heat Integration − Targeting
250
200
150
100
50
Q (kW)
500 15000
MP
HP
0
LP
CW
T' (°C)
Question: Is thisanother Pinch?
T6’ = 50 QC,min = 800
CW
ST
+ 720
- 520
- 1200
+ 180
+ 220
+ 400
T0’ = 260 QH,min = 1000
T1’ = 220 R1 = 1720
T2’ = 210 R2 = 1200
T3’ = 170 R3 = 0
T4’ = 150 R4 = 400
T5’ = 60 R5 = 580
Grand Composite Curve
T. Gundersen Extra 04
Process, Energy and System
Heat Integration − Targeting
250
200
150
100
50
Q (kW)
500 15000
MP
HP
0
LP
CW
T' (°C)
Answer: No
“New” CCs based on Heat Surplus and Deficit Part of Gr.CC and balanced by Hot and Cold Utilities (not representative for Area demand)
T. Gundersen Extra 05
Process, Energy and System
Heat Integration − Targeting
300
250
200
150
100
50
00 1000 1500 2000500 2500
PPUP
UP
CW
MP
HP
LP
T(°C)
Q(kW)
Another way of showing it is not another Process
Pinch
True Balanced Composite Curves with Utilities
(Notice difference in shape and scale)
T. Gundersen Extra 06
Process, Energy and System
Heat Integration − Targeting
T(°C)
Q(kW)
7000
300
250
150
100
50
0
200
6000500040003000200010000
UP
PP
UP