Title: Large Timestep Issues
1Large Timestep Issues
- Lecture 12
- Alessandra Nardi
Thanks to Prof. Sangiovanni, Prof. Newton, Prof.
White, Deepak Ramaswamy, Michal Rewienski, and
Karen Veroy
2Last lecture review
- Transient Analysis of dynamical circuits
- i.e., circuits containing C and/or L
- Examples
- Solution of ODEs (IVP)
- Forward Euler (FE), Backward Euler (BE) and
Trapezoidal Rule (TR) - Multistep methods
- Convergence
- Consistency
3Outline
- Convergence for multistep methods
- Stability
- Region of Absolute Stability
- Dahlquists Stability Barriers
- Stiff Stability (Large timestep issues)
- Examples
- Analysis of FE, BE
- Gears Method
- Variable step size
- More on Implicit Methods
- Solution with NR
- Application of multistep to circuit equations
4Multistep Methods Common AlgorithmsTR, BE, FE
are one-step methods
Multistep Equation
5Multistep Methods Convergence Analysis Two
conditions for Convergence
1) Local Condition One step errors are small
(consistency)
Typically verified using Taylor Series
2) Global Condition The single step errors do
not grow too quickly (stability)
All one-step methods are stable in this sense.
6Multistep Methods StabilityDifference Equation
Why did the best 2-step explicit method fail to
Converge?
Multistep Method Difference Equation
LTE
Global Error
We made the LTE so small, how come the Global
error is so large?
7An Aside on Solving Difference Equations
Consider a general kth order difference equation
Three important observations
8Multistep Methods StabilityDifference Equation
Multistep Method Difference Equation
Definition A multistep method is stable if and
only if
Theorem A multistep method is stable if and only
if
Less than one in magnitude or equal to one and
distinct
9Multistep Methods StabilityStability Theorem
Proof
Given the Multistep Method Difference Equation
are either
If the roots of
- less than one in magnitude
- equal to one in magnitude but distinct
Then from the aside on difference equations
From which stability easily follows.
10Multistep Methods StabilityStability Theorem
Proof
Im
Re
1
-1
11Multistep Methods StabilityA more formal
approach
- Def A method is stable if all the solutions of
the associated difference equation obtained from
(1) setting q0 remain bounded if l?? - The region of absolute stability of a method is
the set of q such that all the solutions of (1)
remain bounded if l?? - Note that a method is stable if its region of
absolute stability contains the origin (q0)
12Multistep Methods StabilityA more formal
approach
Def A method is A-stable if the region of
absolute stability contains the entire left hand
plane (in the ? space)
Im(?)
Re(?)
-1
13Multistep Methods StabilityA more formal
approach
- Each method is associated with two polynomials a
and b - a associated with function past values
- b associated with derivative past values
- Stability roots of a must stay in z?1 and be
simple on z1 - Absolute stability roots of (a-bq) must stay in
z?1 and be simple on z1 when Re(q)lt0.
14Multistep Methods StabilityDahlquists
Stability Barriers
- First For a stable, explicit k-step multistep
method, the maximum number of exactness
constraints that can be satisfied is less than or
equal to k (note there are 2k coefficients). For
implicit methods, the number of constraints that
can be satisfied is either k2 if k is even or
k1 if k is odd. - Second There are no A-stable methods of
convergence order greater than 2, and the
trapezoidal rule is the most accurate.
TR very popular (SPICE)
15Multistep Methods Convergence
AnalysisConditions for convergence Consistency
Stability
1) Local Condition One step errors are small
(consistency)
Exactness Constraints up to p0 (p0 must be gt 0)
2) Global Condition One step errors grow slowly
(stability)
Convergence Result
16Multistep MethodsFE region of absolute stability
Forward Euler
ODE stability region
Im(z)
Difference Eqn Stability region
Region of Absolute Stability
Re(z)
1
-1
17Multistep MethodsBE region of absolute stability
Backward Euler
Im(z)
Difference Eqn Stability region
Re(z)
1
-1
Region of Absolute Stability
18Summary
- Convergence for one-step methods
- Consistency for FE
- Stability for FE
- Convergence for multistep methods
- Consistency (Exactness Constraints)
- Selecting coefficients
- Stability
- Region of Absolute Stability
- Dahlquists Stability Barriers
19Stiff Problems (Large Timestep Issues)Example
- Interval of interest is 0,5
- Uniform step size (for accuracy)
- ? Dt ? 10-6
- ? 5x106 steps !!!
20Stiff Problems (Large Timestep Issues)Example
- Strategy (for previous example) Take 5 steps of
size - 10-6 for accuracy during initial phase and then 5
steps of - size 1.
-
- Stiff problem
- Natural time constants
- Input time constants
- Interval of interest
- If these are widely separated, then the problem
is stiff
21Application ProblemsSignal Transmission in an IC
2x2 example
22Stiff Problems (Large Timestep Issues)FE on two
time-constant circuit
Forward-Euler Computed Solution
The Forward-Euler is accurate for small
timesteps, but goes unstable when the timestep is
enlarged
23Stiff Problems (Large Timestep Issues)BE on two
time-constant circuit
Circuit Example
Backward-Euler Computed Solution
With Backward-Euler it is easy to use small
timesteps for the fast dynamics and then switch
to large timesteps for the slow decay
24Multistep Methods (Large Timestep Issues)BE, FE,
TR on the scalar ODE problem
Scalar ODE
Forward-Euler
Backward-Euler
Trap Rule
25Stiff Problems (Large Timestep Issues)FE on two
time-constant circuit
26Stiff Problems (Large Timestep Issues)BE on two
time-constant circuit
Region of Absolute Stability
Region of Absolute Stability
27Stiff Problems
- We showed that
- The analysis of stiff circuits requires the use
of variable step sizes - Not all the linear multistep methods can be
efficiently used to integrate stiff equations - To be able to choose Dt based only on accuracy
considerations, the region of absolute stability
should allow a large Dt for large time constants,
without being constrained by the small time
constants - Clearly A-stable methods satisfy this requirement
28Backward Differentiation Formula - BDF (Gear
Methods)
- Note that Gears first order method is BE
- It can be shown that
- Gears methods up to order 6 are stiffly stable
and are well-suited for stiff ODEs - Gears methods of order higher than 6 are not
stiffly stable - Less stringent than A-stable
29Gears Method region of absolute
stability(outside the closed curve)
k1
k2
30Gears Method region of absolute
stability(outside the closed curve)
k3
k4
31Variable step size
- When the step size is changed during the
integration, the coefficients of the method need
to be recomputed at each iteration - Example Gears method of order 2
32Variable step size
33More observations
- To minimize the computation time needed to
integrate differential equations, the Dt must be
chosen as large as possible provided that the
desired accuracy is achieved - Several approximation are available. SPICE2 uses
Divided Differences - At a certain time point, different integration
methods would allow different step size - Advantageous to implement a strategy which allows
a change of method as well as of Dt
34Summary on Stiff Stability
- FE timestep is limited by stability and not by
accuracy - BE A-stable, any timestep could be used
- TR most accurate A-stable multistep method
- Gear stiffly stable method (up to order 6)
- The analysis of stiff circuits requires the use
of variable timestep
35Multistep MethodsMore on Implicit Methods
Forward-Euler
Backward-Euler
Requires just function Evaluations
Nonlinear equation solution at each step
36Multistep Implicit MethodsSolution with Newton
Rewrite the multistep Equation
Solve with Newton
Here j is the Newton iteration index
37Multistep Implicit MethodsSolution with Newton
Newton Iteration
Solution with Newton is very efficient
Easy to generate a good initial guess using
polynomial fitting
Jacobian become easy to factor for small timesteps
38Application of linear multistep methods to
circuit equations
39Transient Analysis Flow Diagram
Predict values of variables at tl
Replace C and L with resistive elements via
integration formula
Replace nonlinear elements with G and indep.
sources via NR
Assemble linear circuit equations
Solve linear circuit equations
NO
Did NR converge?
YES
Test solution accuracy
Save solution if acceptable
Select new Dt and compute new integration formula
coeff.
NO
Done?
40Summary
- Transient Analysis of dynamical circuits
- Solution of ODEs (IVP)
- FE, BE and TR
- Multistep methods
- Convergence
- Consistency
- Stability
- Stiff Stability (Large timestep issues)
- Gears method
- Application of multistep to circuit equations
- Did not talk about
- Runge-Kutta
- Predictor-Corrector Methods
41Summary on circuit simulation
- Circuit Equation Formulation
- STA, MNA
- DC Analysis of Nonlinear Circuits
- Solution of Linear Equations (direct and
iterative methods) - Solution of Nonlinear Equations (Newtons
method) - Transient Analysis of Nonlinear Circuits
- Solution of Ordinary Differential Equations- IVP
(multistep methods)
42Appendix to circuit simulation Preconditioners
- The convergence rate of iterative methods depends
on spectral properties of the coefficient matrix.
Hence one may attempt to transform the linear
system into one that is equivalent, but that has
more favorable spectral properties. - A preconditioner is a matrix that effects such a
transformation - Mxb ? A-1MxA-1b
- The choice of a preconditioner is largely
application specific