on the synthesis of correct-by-design embedded control ...lab correct-by-design synthesis a three...
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Lab
On the synthesis of correct-by-designembedded control software
Paulo Tabuada
Cyber-Physical Systems LaboratoryDepartment of Electrical Engineering
University of California at Los Angeles
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 1 / 45
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IntroductionExamples of networked embedded control systems
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 2 / 45
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IntroductionExamples of networked embedded control systems
The OneWireless Plant
Honeywell’s innovative OneWireless™solutions turn valuable data into knowledge, helping plants:
© 2007 Honeywell International, Inc. All rights reserved.
• Keep people, plants and the environment safe • Improve plant and asset reliability • Optimize through efficient employees, equipment and processes
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 3 / 45
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IntroductionExamples of networked embedded control systems
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 4 / 45
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IntroductionExisting paradigm
How are embedded control systems designed today?
Softwaredesign
Softwarevalidation
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 5 / 45
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IntroductionExisting paradigm
Softwaredesign
Softwarevalidation
This iterative scheme has several drawbacks:
Validation by extensive simulation and testingincreases our confidence in the software but fails to provideadequate guarantees of correct operation and performance;
Formal verificationis currently limited to finite state systems and thus cannot beused to verify properties depending on continuous components;
Extensive validation is time consuming thusincreasing the cost and time-to-market of embedded software.
Some of these disadvantages can be mitigated by adopting a correct-by-designapproach to the development of embedded control software.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 6 / 45
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IntroductionExisting paradigm
Softwaredesign
Softwarevalidation
This iterative scheme has several drawbacks:
Validation by extensive simulation and testingincreases our confidence in the software but fails to provideadequate guarantees of correct operation and performance;
Formal verificationis currently limited to finite state systems and thus cannot beused to verify properties depending on continuous components;
Extensive validation is time consuming thusincreasing the cost and time-to-market of embedded software.
Some of these disadvantages can be mitigated by adopting a correct-by-designapproach to the development of embedded control software.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 6 / 45
Lab
Correct-by-design synthesisA three step approach
I shall adopt a three step approach to the synthesis of correct-by-design embeddedcontrol software.
x(t+1)=f(x(t),u(t))dx(t)/dt=f(x(t),u(t))continuous dynamics
finite bisimulation
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 7 / 45
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Correct-by-design synthesisA three step approach
I shall adopt a three step approach to the synthesis of correct-by-design embeddedcontrol software.
x(t+1)=f(x(t),u(t))dx(t)/dt=f(x(t),u(t))continuous dynamics
finite bisimulation hardware+software discrete controller
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 8 / 45
Lab
Correct-by-design synthesisA three step approach
I shall adopt a three step approach to the synthesis of correct-by-design embeddedcontrol software.
x(t+1)=f(x(t),u(t))dx(t)/dt=f(x(t),u(t))continuous dynamics
finite bisimulation hardware+software discrete controller
q(t+1)=g(q(t),x(t))u=k(q(t),x(t))
hybrid controller
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 9 / 45
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Correct-by-design synthesisA three step approach
Ultimately, I would like to:
1 Specify the continuous dynamics;
2 Specify the software+hardware platform;
3 Define the specification;
4 Obtain embedded code enforcing the specification for the continuous dynamicson the given software+hardware platform.
This is a long term goal. Nevertheless, several key ingredients of the proposedapproach are already available. In this talk I will focus on one such ingredient:
Existence of finite approximate bisimulations for control systems.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 10 / 45
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Correct-by-design synthesisA three step approach
Ultimately, I would like to:
1 Specify the continuous dynamics;
2 Specify the software+hardware platform;
3 Define the specification;
4 Obtain embedded code enforcing the specification for the continuous dynamicson the given software+hardware platform.
This is a long term goal. Nevertheless, several key ingredients of the proposedapproach are already available. In this talk I will focus on one such ingredient:
Existence of finite approximate bisimulations for control systems.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 10 / 45
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Key ingredientsControl systems as transition systems
DefinitionA transition system is a quintuple T = (Q, L, - ,O,H), consisting of:
A set of states Q;
A set of inputs L;
A transition relation - ⊆ Q × L×Q;
An output set O;
An output function H : Q → O.
a:=4b:=1while a>0a:=a+bend while
q1
evenq2
odd
e
e
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 11 / 45
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Key ingredientsControl systems as transition systems
DefinitionA transition system is a quintuple T = (Q, L, - ,O,H), consisting of:
A set of states Q;
A set of inputs L;
A transition relation - ⊆ Q × L×Q;
An output set O;
An output function H : Q → O.
a:=4b:=1while a>0a:=a+bend while
q1
evenq2
odd
e
e
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 11 / 45
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Key ingredientsControl systems as transition systems
Can we regard control systems as transition systems?
Definition
A control system is a quadruple Σ = (Rn,U,U , f ), where:
Rn is the state space;
U ⊆ Rm is the input space;
U is “nice” subset of the set of all functions of time from intervals of the form]a, b[⊆ R to U with a < 0 and b > 0;
f : Rn × U → Rn is a “nice” continuous map.
A “nice” curve x :]a, b[→ Rn is said to be a trajectory of Σ if there exists u ∈ Usatisfying x(t) = f (x(t),u(t)), for almost all t ∈ ]a, b[.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 12 / 45
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Key ingredientsControl systems as transition systems
Can we regard control systems as transition systems?
Definition
A control system is a quadruple Σ = (Rn,U,U , f ), where:
Rn is the state space;
U ⊆ Rm is the input space;
U is “nice” subset of the set of all functions of time from intervals of the form]a, b[⊆ R to U with a < 0 and b > 0;
f : Rn × U → Rn is a “nice” continuous map.
A “nice” curve x :]a, b[→ Rn is said to be a trajectory of Σ if there exists u ∈ Usatisfying x(t) = f (x(t),u(t)), for almost all t ∈ ]a, b[.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 12 / 45
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Key ingredientsControl systems as transition systems
Given a control system Σ = (Rn,U,U , f ) and sampling time τ ∈ R+, define thetransition system:
Tτ (Σ) := (Q, L, - ,O,H),
where:
Q = Rn;
L is the set of all the curves in U of duration τ ;
qu- p if x(τ, q,u) = p;
O = Rn;
H = 1Rn .
The output set O = Rn is equipped with the metric d(p, q) = ‖p − q‖.
Can we replace Tτ (Σ) with an equivalent and yet finite transition system?
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 13 / 45
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Key ingredientsControl systems as transition systems
Given a control system Σ = (Rn,U,U , f ) and sampling time τ ∈ R+, define thetransition system:
Tτ (Σ) := (Q, L, - ,O,H),
where:
Q = Rn;
L is the set of all the curves in U of duration τ ;
qu- p if x(τ, q,u) = p;
O = Rn;
H = 1Rn .
The output set O = Rn is equipped with the metric d(p, q) = ‖p − q‖.
Can we replace Tτ (Σ) with an equivalent and yet finite transition system?
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 13 / 45
Lab
Key ingredientsApproximate (bi)simulation
The usual notion of (bi)simulation requires exact matching of outputs.
Definition
Let T1 = (Q1, L1, 1- ,O,H1) and T2 = (Q2, L2, 2
- ,O,H2) be transition systemswith the same output space O. A relation R ⊆ Q1 ×Q2 is said to be a simulationrelation from T1 to T2 if (p1, p2) ∈ R implies:
1 H(p1) = H(p2);
2 p1l11- q1 imply the existence of q2 ∈ Q2 such that p2
l22- q2 with (q1, q2) ∈ R.
Relation R is said to be a bisimulation relation between T1 and T2 if, in addition to 1.and 2., (p1, p2) ∈ R also implies:
3 p2l22- q2 imply the existence of q1 ∈ Q1 such that p1
l11- q1 with (q1, q2) ∈ R.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 14 / 45
Lab
Key ingredientsApproximate (bi)simulation
The usual notion of (bi)simulation requires exact matching of outputs.
Definition
Let T1 = (Q1, L1, 1- ,O,H1) and T2 = (Q2, L2, 2
- ,O,H2) be transition systemswith the same output space O. A relation R ⊆ Q1 ×Q2 is said to be a simulationrelation from T1 to T2 if (p1, p2) ∈ R implies:
1 H(p1) = H(p2);
2 p1l11- q1 imply the existence of q2 ∈ Q2 such that p2
l22- q2 with (q1, q2) ∈ R.
Relation R is said to be a bisimulation relation between T1 and T2 if, in addition to 1.and 2., (p1, p2) ∈ R also implies:
3 p2l22- q2 imply the existence of q1 ∈ Q1 such that p1
l11- q1 with (q1, q2) ∈ R.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 14 / 45
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Key ingredientsApproximate (bi)simulation
Relaxing the equality constraint H(p1) = H(p2) leads to approximate (bi)simulation.
Definition (Girard and Pappas 2005, Tabuada 2005)
Let T1 = (Q1, L1, 1- ,O,H1) and T2 = (Q2, L2, 2
- ,O,H2) be metric transition
systems with the same output space O and let ε ∈ R+. A relation R ⊆ Q1 ×Q2 is saidto be a ε-approximate simulation relation from T1 to T2 if (p1, p2) ∈ R implies:
1 d(H(p1),H(p2)) ≤ ε;
2 p1l11- q1 imply the existence of q2 ∈ Q2 such that p2
l22- q2 with (q1, q2) ∈ R.
Relation R is said to be a bisimulation relation between T1 and T2 if, in addition to 1.and 2., (p1, p2) ∈ R also implies:
3 p2l22- q2 imply the existence of q1 ∈ Q1 such that p1
l11- q1 with (q1, q2) ∈ R.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 15 / 45
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Key ingredientsApproximate (bi)simulation
Relaxing the equality constraint H(p1) = H(p2) leads to approximate (bi)simulation.
Definition (Girard and Pappas 2005, Tabuada 2005)
Let T1 = (Q1, L1, 1- ,O,H1) and T2 = (Q2, L2, 2
- ,O,H2) be metric transition
systems with the same output space O and let ε ∈ R+. A relation R ⊆ Q1 ×Q2 is saidto be a ε-approximate simulation relation from T1 to T2 if (p1, p2) ∈ R implies:
1 d(H(p1),H(p2)) ≤ ε;
2 p1l11- q1 imply the existence of q2 ∈ Q2 such that p2
l22- q2 with (q1, q2) ∈ R.
Relation R is said to be a bisimulation relation between T1 and T2 if, in addition to 1.and 2., (p1, p2) ∈ R also implies:
3 p2l22- q2 imply the existence of q1 ∈ Q1 such that p1
l11- q1 with (q1, q2) ∈ R.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 15 / 45
Lab
Key ingredientsA simple idea
x1 = x2
x2 = u
U = {u−, u0, u+}u−(t) = −1 ∀t ∈ [0, 1]
u0(t) = 0 ∀t ∈ [0, 1]
u+(t) = 1 ∀t ∈ [0, 1]
x2
x1u0
u+
u-
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 16 / 45
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Key ingredientsA simple idea
x1 = x2
x2 = u
U = {u−, u0, u+}u−(t) = −1 ∀t ∈ [0, 1]
u0(t) = 0 ∀t ∈ [0, 1]
u+(t) = 1 ∀t ∈ [0, 1]
x2
x1u0
u0
u+
u-
u+
u+
u-
u-
u0
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 17 / 45
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Key ingredientsA simple idea
x1 = x2
x2 = u
U = {u−, u0, u+}u−(t) = −1 ∀t ∈ [0, 1]
u0(t) = 0 ∀t ∈ [0, 1]
u+(t) = 1 ∀t ∈ [0, 1]
u0
x2
x1
u0
u0 u0
u0 u0
u0
u+ u+
u- u-
u+ u+ u+
u+ u+
u-u-
u-u-u-
Can we extrapolate from this finite transition system?
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 18 / 45
Lab
Key ingredientsA simple idea
x1 = x2
x2 = u
U = {u−, u0, u+}u−(t) = −1 ∀t ∈ [0, 1]
u0(t) = 0 ∀t ∈ [0, 1]
u+(t) = 1 ∀t ∈ [0, 1]
u0
x2
x1
u0
u0 u0
u0 u0
u0
u+ u+
u- u-
u+ u+ u+
u+ u+
u-u-
u-u-u-
Can we extrapolate from this finite transition system?
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 18 / 45
Lab
Key ingredientsA simple idea
x1 = x2
x2 = u
U = {u−, u0, u+}u−(t) = −1 ∀t ∈ [0, 1]
u0(t) = 0 ∀t ∈ [0, 1]
u+(t) = 1 ∀t ∈ [0, 1]
x2
x1
Yes, provided that we know how to robustify it!
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 19 / 45
Lab
Key ingredientsA simple idea
x1 = x2
x2 = u
U = {u−, u0, u+}u−(t) = −1 ∀t ∈ [0, 1]
u0(t) = 0 ∀t ∈ [0, 1]
u+(t) = 1 ∀t ∈ [0, 1]
x2
x1
Yes, provided that we know how to robustify it!
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 20 / 45
Lab
Key ingredientsA simple idea
x1 = x2
x2 = u
U = {u−, u0, u+}u−(t) = −1 ∀t ∈ [0, 1]
u0(t) = 0 ∀t ∈ [0, 1]
u+(t) = 1 ∀t ∈ [0, 1]
x2
x1
Yes, provided that we know how to robustify it!
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 21 / 45
Lab
Key ingredientsIncremental stability
Definition (δ-GAS)A control system Σ is incrementally globally asymptotically stable (δ–GAS) if it isforward complete and there exist a KLa function β such that for any t ∈ R+
0 , anyx , y ∈ Rn and any u ∈ U the following condition is satisfied:
‖x(t , x ,u)− x(t , y ,u)‖ ≤ β(‖x − y‖ , t).
aA continuous function β : R+
0 × R+0 → R+
0 is said to belong to classKL∞ if, for each fixed s, the map β(r, s) is strictlyincreasing, β(0, s) = 0 and β(r, s)→∞ as r →∞, and for each fixed r , the map β(r, s) is decreasing with respect to s andβ(r, s)→ 0 as s →∞.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 22 / 45
Lab
Key ingredientsIncremental stability
Definition (δ-GAS)A control system Σ is incrementally globally asymptotically stable (δ–GAS) if it isforward complete and there exist a KLa function β such that for any t ∈ R+
0 , anyx , y ∈ Rn and any u ∈ U the following condition is satisfied:
‖x(t , x ,u)− x(t , y ,u)‖ ≤ β(‖x − y‖ , t).
aA continuous function β : R+
0 × R+0 → R+
0 is said to belong to classKL∞ if, for each fixed s, the map β(r, s) is strictlyincreasing, β(0, s) = 0 and β(r, s)→∞ as r →∞, and for each fixed r , the map β(r, s) is decreasing with respect to s andβ(r, s)→ 0 as s →∞.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 22 / 45
Lab
Key ingredientsIncremental stability
Definition (δ-GAS)A control system Σ is incrementally globally asymptotically stable (δ–GAS) if it isforward complete and there exist a KLa function β such that for any t ∈ R+
0 , anyx , y ∈ Rn and any u ∈ U the following condition is satisfied:
‖x(t , x ,u)− x(t , y ,u)‖ ≤ β(‖x − y‖ , t).
aA continuous function β : R+
0 × R+0 → R+
0 is said to belong to classKL∞ if, for each fixed s, the map β(r, s) is strictlyincreasing, β(0, s) = 0 and β(r, s)→∞ as r →∞, and for each fixed r , the map β(r, s) is decreasing with respect to s andβ(r, s)→ 0 as s →∞.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 23 / 45
Lab
Key ingredientsIncremental stability
Definition (δ-GAS)A control system Σ is incrementally globally asymptotically stable (δ–GAS) if it isforward complete and there exist a KLa function β such that for any t ∈ R+
0 , anyx , y ∈ Rn and any u ∈ U the following condition is satisfied:
‖x(t , x ,u)− x(t , y ,u)‖ ≤ β(‖x − y‖ , t).
aA continuous function β : R+
0 × R+0 → R+
0 is said to belong to classKL∞ if, for each fixed s, the map β(r, s) is strictlyincreasing, β(0, s) = 0 and β(r, s)→∞ as r →∞, and for each fixed r , the map β(r, s) is decreasing with respect to s andβ(r, s)→ 0 as s →∞.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 24 / 45
Lab
Key ingredientsIncremental stability
Definition (δ-ISS)A control system Σ is incrementally input–to–state stable (δ–ISS) if it is forwardcomplete and there exist a KL function β and a K∞a function γ such that for anyt ∈ R+
0 , any x , y ∈ Rn and any u, v ∈ U the following condition is satisfied:
‖x(t , x ,u)− x(t , y , v)‖ ≤ β(‖x − y‖ , t) + γ(‖u− v‖∞).
aA continuous function γ : R+
0 → R+0 is said to belong to classK∞ if γ is strictly increasing, γ(0) = 0 and γ(r)→∞ as
r →∞.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 25 / 45
Lab
Key ingredientsIncremental stability
Definition (δ-ISS)A control system Σ is incrementally input–to–state stable (δ–ISS) if it is forwardcomplete and there exist a KL function β and a K∞a function γ such that for anyt ∈ R+
0 , any x , y ∈ Rn and any u, v ∈ U the following condition is satisfied:
‖x(t , x ,u)− x(t , y , v)‖ ≤ β(‖x − y‖ , t) + γ(‖u− v‖∞).
aA continuous function γ : R+
0 → R+0 is said to belong to classK∞ if γ is strictly increasing, γ(0) = 0 and γ(r)→∞ as
r →∞.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 26 / 45
Lab
Key ingredientsIncremental stability
1 For linear control systems, that is, x = Ax + Bu, both δ-GAS and δ-ISS areequivalent to stability of A (all the eigenvalues of A have negative real part);
2 In the nonlinear case, by restricting attention to a compact set, GAS impliesδ-GAS and ISS implies δ-ISS;
3 Both δ-GAS and δ-ISS admit Lyapunov characterizations.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 27 / 45
Lab
Main resultsQuantization of control systems
Given a control system Σ = (Rn,U,U , f ), a time quantization τ ∈ R+, a spacequantization η ∈ R+, and an input quantization Uτ ⊆ U , define the transition system:
TηUτ (Σ) := (QηUτ , L, ηUτ
- ,O,H),
where:
QηUτ = [Rn]η;
L = Uτ ;
qu
ηUτ
- p if ‖x(τ, q,u)− p‖ ≤ η2 ;
O = Rn;
H = 1Rn .
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 28 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+, for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
x2
x1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 29 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+, for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
x2
x1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 29 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+, for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
x2
x1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 30 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+, for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
x2
x1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 31 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+, for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
x2
x1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 32 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+, for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
x2
x1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 33 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+ for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
Under the assumptions of the previous theorem, there exists a countable set of controlquanta Uτ rendering TηUτ (Σ) ε-approximate bisimilar to Tτ (Σ).
But how do we compute Uτ?
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 34 / 45
Lab
Main resultsExistence of approximate simulations
Theorem
Let Σ be a control system and let ε ∈ R+ be any desired precision. If Σ is δ-GAS, thenfor any τ ∈ R+ for any Uτ ⊆ U , and for any η ∈ R+ satisfying the following inequality:
β(ε, τ) +η
2≤ ε
there exists an ε-approximate simulation relation R from TηUτ (Σ) to Tτ (Σ) satisfyingR(QηUτ ) = Rn.
Under the assumptions of the previous theorem, there exists a countable set of controlquanta Uτ rendering TηUτ (Σ) ε-approximate bisimilar to Tτ (Σ).But how do we compute Uτ?
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 34 / 45
Lab
Main resultsExistence of approximate bisimulations
Theorem
Let Σ be a digital control system and let ε ∈ R+ be any desired precision. If Σ is δ-ISS,then for any τ ∈ R+, for U(τ) = [U]µ, and for any η ∈ R+ satisfying the followinginequality:
β(ε, τ) +η
2+ γ(µ) ≤ ε
there exists an ε-approximate bisimulation relation R between TηUτ (Σ) and Tτ (Σ).
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 35 / 45
Lab
ExampleA non-holonomic robot
Let us consider the simplest nonholonomic robot:
x = v cos θ (1)
y = v sin θ (2)
θ = ω (3)
and construct a finite abstraction by working on [−2, 2]× [−2, 2]× [0, 2π] and byconsidering constant input curves of duration 3s and assuming values on{0, 1} × {−1.1,−1, 1, 1.1}.
-2 -1 1 2
-2
-1
1
2
-2 -1 1 2
2
4
6
-2 -1 1 2
2
4
6
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 36 / 45
Lab
ExampleA non-holonomic robot
Let us consider the simplest nonholonomic robot:
x = v cos θ (1)
y = v sin θ (2)
θ = ω (3)
and construct a finite abstraction by working on [−2, 2]× [−2, 2]× [0, 2π] and byconsidering constant input curves of duration 3s and assuming values on{0, 1} × {−1.1,−1, 1, 1.1}.
-2 -1 1 2
-2
-1
1
2
-2 -1 1 2
2
4
6
-2 -1 1 2
2
4
6
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 36 / 45
Lab
ExampleA non-holonomic robot
Periodic orbits: find a periodic orbit passing through the origin.
Searching on the discrete abstraction we obtain:
(0, 0, 0.55π)(1,−1.1)- (1.73, 0, 1.47π)
(1,−1)- (0, 0, 0.55π)
0.5 1 1.5
-0.5
0.5
1
0.5 1 1.5
-0.5
0.5
1
0.5 1 1.5 2
-1
-0.5
0.5
1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 37 / 45
Lab
ExampleA non-holonomic robot
Periodic orbits: find a periodic orbit passing through the origin.
Searching on the discrete abstraction we obtain:
(0, 0, 0.55π)(1,−1.1)- (1.73, 0, 1.47π)
(1,−1)- (0, 0, 0.55π)
0.5 1 1.5
-0.5
0.5
1
0.5 1 1.5
-0.5
0.5
1
0.5 1 1.5 2
-1
-0.5
0.5
1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 37 / 45
Lab
ExampleA non-holonomic robot
Language specifications: execute periodic orbits according to the sequence
right→right→left→left→left→right→right→left→left→left.
-2-1
01
-1-0.5
00.5
1
0
2
4
6-1-0.5
00.5
-2 -1 1 2
-1
-0.5
0.5
1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 38 / 45
Lab
ExampleA non-holonomic robot
Language specifications: execute periodic orbits according to the sequence
right→right→left→left→left→right→right→left→left→left.
-2-1
01
-1-0.5
00.5
1
0
2
4
6-1-0.5
00.5
-2 -1 1 2
-1
-0.5
0.5
1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 38 / 45
Lab
ExampleA non-holonomic robot
Switching specifications.
rotate counter-clockwise
rotate clockwise
either clockwise or counter-clockwise
-3 -2 -1 1 2 3
-1
-0.5
0.5
1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 39 / 45
Lab
ExampleA non-holonomic robot
Switching specifications.
rotate counter-clockwise
rotate clockwise
either clockwise or counter-clockwise
-3 -2 -1 1 2 3
-1
-0.5
0.5
1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 39 / 45
Lab
ExampleA non-holonomic robot
Switching specifications.
rotate counter-clockwise
rotate clockwise
either clockwise or counter-clockwise
-3 -2 -1 1 2 3
-1
-0.5
0.5
1
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 40 / 45
Lab
ExampleA non-holonomic robot
Interaction with discrete signals.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 41 / 45
Lab
Putting the pieces togetherAbstraction
x(t+1)=f(x(t),u(t))dx(t)/dt=f(x(t),u(t))continuous dynamics
finite bisimulation
The abstraction step can be done for a reasonable class of control systems;
Recent results eliminate the stability assumption by ensuring only the existenceof approximate alternating simulation relations;
Multi-resolution quantization and other techniques can be used to reduce thesize of the abstractions.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 42 / 45
Lab
Putting the pieces togetherSynthesis of discrete controllers
x(t+1)=f(x(t),u(t))dx(t)/dt=f(x(t),u(t))continuous dynamics
finite bisimulation hardware+software discrete controller
Synthesis of controllers based on language specifications can be done byresorting to supervisory control or algorithmic game theory;
Synthesis of controllers based on (bi)simulation specifications can be done bymodifying existing algorithms for the construction of (bi)simulations;
Incorporating timing considerations is crucial to address real-time issues.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 43 / 45
Lab
Putting the pieces togetherController refinement
x(t+1)=f(x(t),u(t))dx(t)/dt=f(x(t),u(t))continuous dynamics
finite bisimulation hardware+software discrete controller
q(t+1)=g(q(t),x(t))u=k(q(t),x(t))
hybrid controller
The refinement of discrete to hybrid controllers is based on the approximatebisimulation relation between the discrete abstraction and the continuous plant;
The hybrid controller is a formal model for embedded code. Automated codegeneration from this model is conceptually simple;
Correctness of operation depends on real-time scheduling and many otherconsiderations.
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 44 / 45
Lab
Questions?
Many questions remain open and much work is to be done before we can synthesizecorrect-by-design embedded control software.
The ingredients, however, are becoming available.
The work described in this talk was the result of:
the dedication of my students and postdocs: Giordano Pola (now AssistantProfessor at University of L’Aquila), Manuel Mazo Jr., and Anna Davitian;
the inspiring discussions with my collaborators: Aaron Ames, Antoine Girard,Agung Julius, Rupak Majumdar, and George Pappas;
the financial support from the National Science Foundation.
For papers and more information:http://www.cyphylab.ee.ucla.edu/
http://www.ee.ucla.edu/∼tabuada
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 45 / 45
Lab
Questions?
Many questions remain open and much work is to be done before we can synthesizecorrect-by-design embedded control software.
The ingredients, however, are becoming available.
The work described in this talk was the result of:
the dedication of my students and postdocs: Giordano Pola (now AssistantProfessor at University of L’Aquila), Manuel Mazo Jr., and Anna Davitian;
the inspiring discussions with my collaborators: Aaron Ames, Antoine Girard,Agung Julius, Rupak Majumdar, and George Pappas;
the financial support from the National Science Foundation.
For papers and more information:http://www.cyphylab.ee.ucla.edu/
http://www.ee.ucla.edu/∼tabuada
Paulo Tabuada (CyPhyLab - UCLA) Berkeley 04/17/09 45 / 45