On 3/12/16 8:37 PM, Matthew Knepley wrote:
On Sat, Mar 12, 2016 at 8:34 PM, Emil Constantinescu
<emcon...@mcs.anl.gov <mailto:emcon...@mcs.anl.gov>> wrote:
I also find it useful to go through one of the simple examples
available for TS:
http://www.mcs.anl.gov/petsc/petsc-current/src/ts/examples/tutorials/index.html
(ex8 may be a good start).
As Barry suggested, you need to implement IFunction and IJacobian.
The argument "u" is S_o, S_w, and p stacked together and "u_t"
their corresponding time derivatives. The rest is calculus, but
following an example usually helps a lot in the beginning.
Are you guys saying that IFunction and IJacobian are enough to do the
adjoint system as well?
Pretty much yes, but it depends on the cost function. This is the beauty
of discrete adjoints - if you have the Jacobian (transpose, done
internally through KSP) you're done. You need IJacobian for sure to do
the backward propagation. If you have that, the rest is usually trivial.
Mr. Hong Zhang (my postdoc) set up quite a few simple examples.
Emil
Matt
Out of curiosity, what is the application?
Emil
On 3/12/16 3:19 PM, Barry Smith wrote:
This is only a starting point, Jed and Emil can fix my
mistakes and provide additional details.
In your case you will not provide a TSSetRHSFunction and
TSSetRHSJacobian since everything should be treated implicitly
as a DAE.
First move everything in the three equations to the left
side and then differentiate through the \partial/\partial t so
that it only applies to the S_o, S_w, and p. For example for the
first equation using the product rule twice you get something like
\phi( p ) \rho_o( p ) \partial S_o/ \partial t + phi( p )
S_o \partial \rho_o( p ) \partial t + \rho_o( p ) S_o
\partial \phi( p ) \partial t - F_o = 0
\phi( p ) \rho_o( p ) \partial S_o/ \partial t + phi( p )
S_o \rho_o'(p) \partial p \partial t + \rho_o( p ) S_o \phi'( p
) \partial p \partial t - F_o = 0
The two vector arguments to your IFunction are exactly the S_o,
S_w, and p and \partial S_o/ \partial t , \partial S_w/
\partial t, and \partial p/ \partial t so it is immediate to
code up your IFunction once you have the analytic form above
For the IJacobian and the "shift business" just remember that
dF/dU means take the derivative of the IFunction with respect to
S_o, S_w, and p treating the \partial S_o/ \partial t ,
\partial S_w/ \partial t, and \partial p/ \partial t as if they
were independent of S_o, S_w, and p. For the dF/dU_t that means
taking the derivate with respect to the \partial S_o/ \partial t
, \partial S_w/ \partial t, and \partial p/ \partial t
treating the S_o, S_w, and p as independent of \partial S_o/
\partial t , \partial S_w/ \partial t, and \partial p/
\partial t. Then you just need to form the sum of the two
parts with the a "shift" scaling dF/dU + a*dF/dU_t
For the third equation everything is easy. dF/dS_o = 1 dF/dS_w =
1 dF/dp = 0 dF/d (\partial S_o)/\partial t = 0 (\partial
S_w)/\partial t = 0 (\partial p)/\partial t = 0
Computations for the first two equations are messy but
straightforward. For example for the first equation dF/dS_o =
phi( p ) \rho_o'(p) \partial p \partial t + \rho_o( p ) \phi'(
p ) \partial p + dF_o/dS_o and dF/d (\partial S_o)/\partial t)
= \phi( p ) \rho_o( p )
Barry
On Mar 12, 2016, at 12:04 PM, Matthew Knepley
<knep...@gmail.com <mailto:knep...@gmail.com>> wrote:
On Sat, Mar 12, 2016 at 5:41 AM, Max la Cour Christensen
<ml...@dtu.dk <mailto:ml...@dtu.dk>> wrote:
Hi guys,
We are making preparations to implement adjoint based
optimisation in our in-house oil and gas reservoir
simulator. Currently our code uses PETSc's DMPlex, Vec, Mat,
KSP and PC. We are still not using SNES and TS, but instead
we have our own backward Euler and Newton-Raphson
implementation. Due to the upcoming implementation of
adjoints, we are considering changing the code and begin
using TS and SNES.
After examining the PETSc manual and examples, we are still
not completely clear on how to apply TS to our system of
PDEs. In a simplified formulation, it can be written as:
\partial( \phi( p ) \rho_o( p ) S_o )/ \partial t = F_o(p,S)
\partial( \phi( p ) \rho_w( p ) S_w )/ \partial t = F_w(p,S)
S_o + S_w = 1,
where p is the pressure,
\phi( p ) is a porosity function depending on pressure,
\rho_x( p ) is a density function depending on pressure,
S_o is the saturation of oil,
S_g is the saturation of gas,
t is time,
F_x(p,S) is a function containing fluxes and source terms.
The primary variables are p, S_o and S_w.
We are using a lowest order Finite Volume discretisation.
Now for implementing this in TS (with the prospect of later
using TSAdjoint), we are not sure if we need all of the
functions: TSSetIFunction, TSSetRHSFunction, TSSetIJacobian
and TSSetRHSJacobian and what parts of the equations go
where. Especially we are unsure of how to use the concept of
a shifted jacobian (TSSetIJacobian).
Any advice you could provide will be highly appreciated.
Barry and Emil,
I am also interested in this, since I don't know how to do it.
Thanks,
Matt
Many thanks,
Max la Cour Christensen
PhD student, Technical University of Denmark
--
What most experimenters take for granted before they begin
their experiments is infinitely more interesting than any
results to which their experiments lead.
-- Norbert Wiener
--
What most experimenters take for granted before they begin their
experiments is infinitely more interesting than any results to which
their experiments lead.
-- Norbert Wiener
