Universität Stuttgart Modeling Multi-Element Systems Using Bond Graphs 1.Introduction 2.Mixture...
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Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Modeling Multi-Element SystemsUsing Bond Graphs
Modeling Multi-ElementModeling Multi-Element SystemsSystemsUsing Bond GraphsUsing Bond Graphs
Jürgen GreifenederFrançois E. Cellier
18.10.2001
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
1. Introduction• Review• Basics of Multi-Element Systems
2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
Contents
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Introduction
• Describing a thermodynamical problem necessitates 3 variables.
• Separation in storage and dissipative elements. Storage elements calculate the potentials and therefore need to know about the matter, they are representing. Dissipative elements calculate flows and do not care, which matter they are dealing with (network theory).
• Elements do not know about each other.
• No quasi-stationary or flow-equilibrium assumptions were made.
• Contrary to earlier efforts in this field, this work delt with real, rather than pseudo bond graphs.
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
pq
TS
g
M
.
.
0
0 0
CFCF
C C
C Ø3
CFCF
Icon:
The C-field (storage element)
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
CFCF1CFCF2
3 3CD
CFCF1CFCF2
3 3DVAVolume work:
Conduction:
Ø Ø3RF
3
33
CFCF1 CFCF2
, s1 1 , s2 2Convection:
Basic dissipative Elements
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Traditional Thermodynamics
One Temperature, one pressure and n partial mass’ => n+2 equations.
pq
0
0 0
CFCF
C C
CC
TS
.
0 00 ....g
1M1
.g2M
2
.g3M3
.
g n
M n.....
1 2 3 n
n
Ø
?
CFCF
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Multi-Element Mono-Phase Systems
CF1Ø
3
3
CF2
3Ø
2 2DVACD
CF3
Ø
DVA
CD
2
2
DVACD
2
2
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Ideal and Non-Ideal Mixtures
• In the process of mixing, additionally entropy will be created, which must be distributed among the participating components
• Distribution is a function of the molar fractions
• CF-Elements are not supposed to know about each other only necessary information will be provided
CF1 CF2MIMI
{M1}
{x1
{M2}
{x2
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Ideal and Non-Ideal Mixtures
• In the process of mixing, additionally entropy will be created, which must be distributed among the participating components
• Distribution is a function of the molar fractions
• CF-Elements are not supposed to know about each other only necessary information will be provided
CF1CF2MIMI
{M1, V1, S1}
{x1s1Exv1
Ex
{M2, V2, S2}
{x2s2Exv2
Ex
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Entropy of Mixing
TS.
pq 11
1
1
11
g1(T,p)11M
.1
TS.
pq
1
1
g1 (T,p)
M.
1
mix
TRSM.
1
g1
Sid
mix
1
CFCF11 CFCF12
TS.
pq 11
2
2
11
g2(T,p)11M
.2
TS.
pq
2
2
g2 (T,p)
M.
2
mix
TRSM.
2
g2
Sid
mix
2
CFCF21 CFCF22
MIMI
x21
x11
M21
M11
CDDVA.
.
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
T2
S.
p2
q 112
2
11
g2(T2,p2) 11M.
2
T2mix
S.
p2mix
q
2
2
g2 (T2,p2)
M2
.mix
CFCF 21 CFCF 22
MIMI CDDVA
RS
M.
2g2
S2
.RS mRS
0
p2
T2
q2
S2
.
T2mix
T1
S.
p1
q 111
1
11
g1 (T1,p1) 11M.
1
T1mix
S.
p1mix
q
1
1g1 (T1,p1)
M1
.mix
CFCF 11
RS
M.
1
g1
S1
.RS mRS
0
p1
T1
q1
S1
.
T1mix
CFCF 12
An François: eigentlich müßte ich hier erwähnen, daß die drei (m)RS-Elemente einem RF-Element entsprechen (vor allem, weil dies auf der nächsten Folie verwendet wird). Allerdings habe ich die interne RF-Struktur nie verwendet und sehe dies auch nicht als erforderlich an.
Daher: Was tun? Die nächste Folie rauslassen?
An François: eigentlich müßte ich hier erwähnen, daß die drei (m)RS-Elemente einem RF-Element entsprechen (vor allem, weil dies auf der nächsten Folie verwendet wird). Allerdings habe ich die interne RF-Struktur nie verwendet und sehe dies auch nicht als erforderlich an.
Daher: Was tun? Die nächste Folie rauslassen?
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
CFCF12
CFCF22
MIMI CDDVA
Ø Ø3RF
3
CFCF11
Ø Ø3RF
3
CFCF21
3
3
3
3
3CD
DVA
3
CDDVA
Øoutside
3
3
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Convection in Multi-Element Systems
CF12
CF13
CF11
Ø
3
3
3
3
3
Ø
Ø
3
DVACD
3
3
CDDVA CF22
CF23
CF21
3
3
3
3
3
Ø
Ø
Ø
3
DVACD
3
3DVACD
3
CDDVA
3
DVACD
3RF
DVACD
3
3 3RFDVACD
3 3RFDVACD
horizontalExchange(transport)
verticalExchange(mixture)
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Two-Element, Two-Phase, Two-Compartment Convective System
Gas
CF11
Fl.
CF11
Fl.
CF21
Gas
CF21
Ø
3
3
3
3
3
Ø
Ø
Ø
3
DVACD
3
CDCondensation/Evaporation
DVA
3
3
3
3
CDCondensation/Evaporation
DVA
Gas
CF12
Fl.
CF12
Fl.
CF22
Gas
CF22
Ø3
3
3
3
3
3
Ø
Ø
Ø
3
DVACD
3
CDCondensation/Evaporation
DVA
3
3
3DVACD
3
CDCondensation/Evaporation
DVA
3
DVACD
3RF
DVACD
3
3 3
3 3
CDDVARF
CDDVARF
3 3RF
DVACD
phase-boundary
3
DVACD
3
3
DVACD
3
3
DVACD
3
3
DVACD
3
MIMI{x21, S
E
21, VE
21}
{M21, T21, p 21} MIMI1 2
+
Vge
s
+
Vge
s
{M11, T
11, p
11}
{x21,
SE
21,
VE
21}
{M12, T
12, p
12}
{x12,
SE
12,
VE
12}
{M22, T22, p 22}
{x22, SE
22, VE
22}
An François:
Wie genau muß ich auf diese Abbildung eingehen?
An François:
Wie genau muß ich auf diese Abbildung eingehen?
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Equilibration of Concentrations
CFCFii
3
Ø 3 3CDDVAKA
3
Ø
CFCFi+1i+1
33... ...
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Model of a Pressure Cooker
water
air
steam
SE: 393 K
CD (t)
KV
DVA
DVA
CD
CD
CD DVA
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
water
air
steam
KV
DVA
DVA
CD
CD
CD DVA
KV
Air in boundary
layer
Steam in boundary
layer
CD
RF: p
RF: p
CD
CDDVA
CD
CD
SE: 293 K
CD (t)
CD (t)
SE: 393 K
CD (t)
CD (t)
CD (t)
Model of a Pressure Cooker
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Temperature Graphs
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Pressure Graphs
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Humidity Graphs
OHsat
partialsteam
p
p2
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Mass Fraction Graphs
airsteam
steam
mm
m
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Conclusion
• The elements introduced suffice to model most thermodynamical problems
• Modeling each matter separately as a storage element and connecting them by means of dissipative elements (RF-concept) simplyfies the modeling task, offers insight into physical functioning of multi-element systems and leads to mathematical models that can be simulated in a numerically stable and highly accurate fashion.
• Models are still limited to systems without chemical reactions
Universität Stuttgart
Modeling Multi-Element SystemsModeling Multi-Element SystemsUsing Bond GraphsUsing Bond Graphs
1. Introduction2. Mixture Properties3. Transport Phenomena4. Model of a Pressure Cooker5. Conclusions
University of Arizona
18. Oktober 2001Jürgen Greifeneder, François Cellier
Danke
Ende
Thank you!Thank you!RemerRemerciement!ciement!
Jürgen GreifenederFrançois E. Cellier