I'm an engineering student. Pretty much all math I have to do is something in R2 or R3 and concerns differential geometry. Naturally I really like sympy because it makes my calculations reusable and presentable.
What I found:
The thing in sympy that comes closeset to what I know functions as, which is as mapping of scalar or vector values to scalar or vector values, with a name and connected to an expressions seems to be something of the form
functionname=sympy.Lambda(Variables in tuple, Expression)
or as an example
f=sympy.Lambda((x),x+1)
I also found that sympy has the diffgeom module that defines Manifolds, Patches and can then perform some operations on functions without expressions or points. Like translating a point in a coordinate system to the same point in a different, linked coordinate system.
I haven't found a way to perform those operations and transformations on functions like those above. Or to define something in the diffgeom context that performs like the Lambda function.
Examples of what I'd like to do:
scalarfield f (x,y,z) = expression
grad (f) = ( d expression / dx , d expression / dy , d expression / dz)^T
vectorfield v (x,y,z) = ( expression 1 , expression 2 , expression 3 )^T
I'd then like to be able to integrate the vectorfield over bodies or curves.
Do these things exist and I haven't found them?
Are they doable with diffgeom and I didn't understand it?
Would I have to write this myself with the backbones that sympy already provides?
There is a differential geometry module within sympy:
http://docs.sympy.org/latest/modules/diffgeom.html
For more examples you can see http://blog.krastanov.org/pages/diff-geometry-in-python.html
To do the suggested in the diffgeom module, just define your expression using the base coordinates of your manifold:
from diffgeom.rn import R2
scalar = (R2.r**2 - R2.x**2 - R2.y**2) # you can mix coordinate systems
gradient = (R2.e_x + R2.e_y).rcall(scalar)
There are various functions for change of coordinates, etc. Probably many things are missing, but it would take usage and bug reports (and help) for all this to get implemented.
You can see some other examples in the test files:
tested examples from a text book https://github.com/sympy/sympy/blob/master/sympy/diffgeom/tests/test_function_diffgeom_book.py
more tests https://github.com/sympy/sympy/blob/master/sympy/diffgeom/tests/test_diffgeom.py
However for doing what is suggested in your question, doing it through differential geometry (while possible) would be an overkill. You can just use the matrices module:
def gradient(expr, vars):
return Matrix([expr.diff(v) for v in vars])
More fancy things like matrix jacobians and more are implemented.
A final remark: using expressions instead of functions and lambdas will probably result in more readable and idiomatic sympy code (often it is more natural to use subs to substitute a symbols instead of some kind of closure, lambda, function call, etc).
Related
Apologies in advance for how vague this question is (unfortunately I don't know enough about how jax tracing works to phrase it more precisely), but: Is there a way to completely insulate a function or code block from jax tracing?
For context, I have a function of the form:
def f(x, y):
z = h(y)
return g(x, z)
Essentially, I want to call g(x, z), and treat z as a constant when doing any jax transformations. However, setting up the argument z is very awkward, so the helper function h is used to transform an easier-to-specify input y into the format required by g. What I'd like is for jax to treat h as a non-traceable black box, so that doing jit(lambda x: f(x, y0)) for a particular y0 is the same as first computing z0 = h(y0) with numpy, then doing jit(lambda x: g(x, z0)) (and similar with grad or whatever other function transformations).
In my code, I've already written h to only use standard numpy (which I thought might lead to black-box behaviour), but the compile time of jit(lambda x: f(x, y0)) is noticeably longer than the compile time of jit(lambda x: g(x, z0)) for z0 = h(y0). I have a feeling the compile time may have something to do with jax tracing the many loops in h, though I'm not sure.
Some additional notes:
Writing h in a jax-friendly way would be awkward (input formatting is ragged, tons of looping/conditionals, output shape dependent on input value, etc) and ultimately more trouble than it's worth as the function is extremely cheap to execute, and I don't ever need to differentiate it (the input data is integer-based).
Thoughts?
Edit addition for clarity: I know there are maybe ways around this if, e.g. f is a top-level function. In this case it isn't such a big deal to get the user to call h first to "pre-compile" the jax-friendly inputs to g, then freely perform whatever jax transformations they want to lambda x: g(x, z0). However, I'm imagining cases in which we have many functions that we want to chain together, that have the same structure as f, where there are some jax-unfriendly inputs/computations, but these inputs will always be treated as constant to the jax part of the computation. In principle one could always pull out these pre-computations to set up the jax stuff, but this seems difficult if we have a non-trivial collection of functions of this type that will be calling each other.
Is there some way to control how f gets traced, so that while tracing it knows to just evaluate z=h(y) (instead of tracing h) then continue with tracing g(x, z)?
f_jitted = jax.jit(f, static_argnums=1)
static_argnums parameter probably could help
https://jax.readthedocs.io/en/latest/notebooks/Common_Gotchas_in_JAX.html
You can use transformation parameters such as static_argnums for jit to avoid tracing particular arguments of transformed functions, though at the cost of more recompiles.
I am getting a function (a learned dynamical system) through a neural network and want to pass it to JiTCODE to calculate trajectories, Lyapunov exponents, etc. As per the JiTCODE documentation, the function f has to be a symbolic function. Is there any way to change this since ultimately JiTCODE is going to lambdify the symbolic function?
Basically, this is what I'm doing right now:
# learns derviates from the Neural net model
# returns an array of numbers [\dot{x},\dot{y}] for input [x,y]
learned_fn = lambda t, y0: NN_model(t, y0)
ODE = jitcode_lyap(learned_fn, n_lyap=2)
ODE.set_integrator("vode")
First beware that JiTCODE does not take regular functions like your learned_fn as an input. It takes either iterables of symbolic expressions or generator functions returning symbolic expressions. This is why your example code will likely produce an error.
What you are asking for
You can “inject” any derivative with the right signature into JiTCODE by changing the f property and telling it that it failed compiling the actual derivative. Here is a minimal example doing this:
from jitcode import jitcode, y
ODE = jitcode([0])
ODE.f = lambda t,y: y[0]
ODE.compile_attempt = False
ODE.set_integrator("dopri5")
ODE.set_initial_value([1],0.0)
for time in range(30):
print(time,*ODE.integrate(time))
Why you probably do not want to do this
Ignoring Lyapunov exponents for a second, the entire point of JiTCODE is to hard-code your derivative for you and pass it to SciPy’s ode or solve_ivp who perform the actual integration. Thus the above example code is just an overly complicated way of passing a function to one SciPy’s standard integrators (here ode), with no advantage. If your NN_model is very efficiently implemented in the first place, you may not even gain a speed boost from JiTCODE’s auto-compilation.
The main reason to use JiTCODE’s Lyapunov-exponent capabilities is that it automatically obtains the Jacobian and the ODE for the tangent-vector evolution (needed for the Benettin method) from the symbolic representation of the derivative. Without a symbolic input, it cannot possibly do this. You could theoretically inject a tangent-vector ODE as well, but then again you would leave little for JiTCODE to do and you would probably better off using SciPy’s ode or solve_ivp directly.
What you probably need
If you want to use JiTCODE, you need to write a small piece of code that translates the output of your neural-network training to a symbolic representation of your ODE as needed by JiTCODE. This is probably much less scary than it sounds. You just need to obtain the trained coefficients and insert it in the equations of the general form of the neural network.
If you are lucky and your NN_model fully supports duck typing (and ), you may do something like this:
from jitcode import t,y
n = 10 # dimension of your ODE
NN_input = [y(i) for i in range(n)]
learned_fn = NN_model(t,NN_input)[1]
The idea is that you feed NN_model once with abstract symbolic input (t and NN_input). NN_model then once acts on this abstract input providing you an abstract result (here you need the duck-typing support). If I interpreted the output of your NN_model correctly, the second component of this result should be the abstract derivative as required by JiTCODE as an input.
Note that your NN_model appears to expect dimensions to be indices, but JiTCODE’s y expects dimensions to be function arguments. Thus you cannot just choose NN_input = y, but you have to transform it as above.
To quote directly from the linked documentation
JiTCODE takes an iterable (or generator function or dictionary) of symbolic expressions, which it translates to C code, compiles on the fly,
so there is no lambdification going on, the function is parsed, not just evaluated.
But in general that should be no problem, you just use the JITCODE provided symbolic vector y and symbol t instead of the function arguments t,y of the right side of the ODE.
I am trying to Maximize 10 very long linear equations, All equations are similar except for one variable (say Z).
I was thinking of putting a single equation inside a function and pass Z as a parameter.
Can we optimise the python functions?
I have looked into pyomo,pulp,cvxpy documentations and haven't found any code samples. which makes me think it this isn't possible
#This is what currently it is
Maximize
(X*fun(1,Z)) + (X2*fun(1,Z)) + ...
(X*fun(1,Z1)) + (X2*fun(1,Z1)) + ...
..
..
Solve for
X1 and X2
#This an example what I am trying to do
Def optimise(Z):
(X*fun(1,Z)) + (X2*fun(1,Z)) + ...
Maximize
optimise(13)
optimise(24)
optimise(34)
optimise(14)
optimise(12)
optimise(11) #is optimizing with funtions possible ?
Solve for
X1 and X2
It depends on what your function returns. Pyomo is an algebraic modeling language and requires access to the full algebraic equations. If your Python function returns an expression involving Pyomo Var components then it should work. If the function simply returns a value depending on the current value of a Pyomo Var then it will not work. You need to provide more details on the function and the model you're trying to solve for us to say for sure if it's supported or not.
For a few months I started working with python, considering the great advantages it has. But recently, i used odeint from scipy to solve a system of differential equations. But during the integration process the implemented function doesn't work as expected.
In this case, I want to solve a system of differential equations where one of the initial conditions (x[0]) varies (between 4-5) depending on the value that the variable reaches during the integration process (It is programmed inside of the function by means of the if structure).
#Control of oxygen
SO2_lower=4
SO2_upper=5
if x[0]<=SO2_lower:
x[0]=SO2_upper
When the function is used by odeint, some lines of code inside the function are obviated, even when the functions changes the value of x[0]. Here is all my code:
import numpy as np
from scipy.integrate import odeint
import matplotlib.pyplot as plt
plt.ion()
# Stoichiometric parameters
YSB_OHO_Ox=0.67 #Yield for XOHO growth per SB (Aerobic)
YSB_Stor_Ox=0.85 #Yield for XOHO,Stor formation per SB (Aerobic)
YStor_OHO_Ox=0.63 #Yield for XOHO growth per XOHO,Stor (Aerobic)
fXU_Bio_lys=0.2 #Fraction of XU generated in biomass decay
iN_XU=0.02 #N content of XU
iN_XBio=0.07 #N content of XBio
iN_SB=0.03 #N content of SB
fSTO=0.67 #Stored fraction of SB
#Kinetic parameters
qSB_Stor=5 #Rate constant for XOHO,Stor storage of SB
uOHO_Max=2 #Maximum growth rate of XOHO
KSB_OHO=2 #Half-saturation coefficient for SB
KStor_OHO=1 #Half-saturation coefficient for XOHO,Stor/XOHO
mOHO_Ox=0.2 #Endogenous respiration rate of XOHO (Aerobic)
mStor_Ox=0.2 #Endogenous respiration rate of XOHO,Stor (Aerobic)
KO2_OHO=0.2 #Half-saturation coefficient for SO2
KNHx_OHO=0.01 #Half-saturation coefficient for SNHx
#Other parameters
DT=1/86400.0
def f(x,t):
#Control of oxygen
SO2_lower=4
SO2_upper=5
if x[0]<=SO2_lower:
x[0]=SO2_upper
M=np.matrix([[-(1.0-YSB_Stor_Ox),-1,iN_SB,0,0,YSB_Stor_Ox],
[-(1.0-YSB_OHO_Ox)/YSB_OHO_Ox,-1/YSB_OHO_Ox,iN_SB/YSB_OHO_Ox-iN_XBio,0,1,0],
[-(1.0-YStor_OHO_Ox)/YStor_OHO_Ox,0,-iN_XBio,0,1,-1/YStor_OHO_Ox],
[-(1.0-fXU_Bio_lys),0,iN_XBio-fXU_Bio_lys*iN_XU,fXU_Bio_lys,-1,0],
[-1,0,0,0,0,-1]])
R=np.matrix([[DT*fSTO*qSB_Stor*(x[0]/(KO2_OHO+x[0]))*(x[1]/(KSB_OHO+x[1]))*x[4]],
[DT*(1-fSTO)*uOHO_Max*(x[0]/(KO2_OHO+x[0]))*(x[1]/(KSB_OHO+x[1]))* (x[2]/(KNHx_OHO+x[2]))*x[4]],
[DT*uOHO_Max*(x[0]/(KO2_OHO+x[0]))*(x[2]/(KNHx_OHO+x[2]))*((x[5]/x[4])/(KStor_OHO+(x[5]/x[4])))*(KSB_OHO/(KSB_OHO+x[1]))*x[4]],
[DT*mOHO_Ox*(x[0]/(KO2_OHO+x[0]))*x[4]],
[DT*mStor_Ox*(x[0]/(KO2_OHO+x[0]))*x[5]]])
Mt=M.transpose()
MxRm=Mt*R
MxR=MxRm.tolist()
return ([MxR[0][0],
MxR[1][0],
MxR[2][0],
MxR[3][0],
MxR[4][0],
MxR[5][0]])
#ODE solution
t=np.linspace(0.0,3600,3600)
#Initial conditions
y0=np.array([5,176,5,30,100,5])
Var=odeint(f,y0,t,args=(),h0=1,hmin=1,hmax=1,atol=1e-5,rtol=1e-5)
Sol=Var.tolist()
plt.plot(t,Var[:,0])
Thanks very much in advance!!!!!
Short answer:
You should not modify input state vector inside your ODE function. Instead try the following and verify your results:
x0 = x[0]
if x0<=SO2_lower:
x0=SO2_upper
# use x0 instead of x[0] in the rest of this function body
I suppose that this is your problem, but I am not sure, since you did not explain what exactly was wrong with the results. Moreover, you do not change "initial condition". Initial condition is
y0=np.array([5,176,5,30,100,5])
you just change the input state vector.
Detailed answer:
Your odeint integrator is probably using one of the higher order adaptive Runge-Kutta methods. This algorithm requires multiple ODE function evaluations to calculate single integration step, therefore changing the input state vector may lead to undefined results. In C++ boost::odeint this is even not possible to do so, because input variable is "const". Python however is not as strict as C++ and I suppose that it is possible to make this kind of bug unintentionally (I did not try it, though).
EDIT:
OK, I understand what you want to achieve.
Your variable x[0] is constrained by modular algebra and it is not possible to express in the form
x' = f(x,t)
which is one of the possible definitions of the Ordinary Differential Equation, that ondeint library is meant to solve. However, few possible "hacks" can be used here to bypass this limitation.
One possibility is to use a fixed step and low order (because for higher order solvers you need to know, which part of the algorithm you are actually in, see RK4 for example) solver and change your dx[0] equation (in your code it is MxR[0][0] element) to:
# at the beginning of your system
if (x[0] > S02_lower): # everything is normal here
x0 = x[0]
dx0 = # normal equation for dx0
else: # x[0] is too low, we must somehow force it to become S02_upper again
dx0 = (x[0] - S02_upper)/step_size // assuming that x0_{n+1} = x0_{n} + dx0*step_size
x0 = S02_upper
# remember to use x0 in the rest of your code and also remember to return dx0
However, I do not recommend this technique, because it makes you strongly dependent on the algorithm and you must know the exact step size (although, I may recommend it for saturation constraints). Another possibility is to perform a single integration step at a time and correct your x0 each time it is necessary:
// 1 do_step(sys, in, dxdtin, t, out, dt);
// 2 do something with output
// 3 in = out
// 4 return to 1 or finish
Sorry for C++ syntax, here is the exhaustive documentation (C++ odeint steppers), and here is its equivalent in python (Python ode class). C++ odeint interface is better for your task, however you may achieve exactly the same in python. Just look for:
integrate(t[, step, relax])
set_initial_value(y[, t])
in docs.
This question regards making sympy's geometric algebra module use both covariant and contravariant vector forms to make the output much more compact. So far I am able to use one or the other, but not both together. It may be that I don't know the maths well enough, and the answer is in the documentation after all.
Some background:
I have a system of equations that I want to solve in a complicated non-orthogonal coordinate system. The metric tensor elements of this coordinate system are known, but their expressions are unwieldy so I'd like to to keep them hidden and simply use gij, the square root of its determinant J, and gij. Also it's useful to describe vectors, V, in either their contravariant or their covariant forms,
V = ∑Viei = ∑Viei,
and transform between them where necessary.
Here ei = ∇u(i) and u(i) is the ith coordinate, and ei = ∂R/∂u(i).
This notation is the same as that used in this invaluable text, which I cannot recommend more. Specifically, chapter 2 will be useful for this question.
There are many curls and divergence operations in the system of equations I'm trying to solve. The former is most simply expressed with the contravariant form of the a vector, and the latter with the covariant:
∇.V = 1/J ∑∂u(i)JVi,
∇ x V = εijk/J (∂u(i)Vi)ei,
where εijk is the Levi-Cevitta symbol. I would consider this question answered if I could print the above two equations using sympy's geometric algebra module.
How does one configure sympy's geometric algebra module to express calculations in this manner i.e. using covariant and contravariant vector expressions in order to hide away the complicated nature of the coordinate system?
Maybe there is an alternative toolbox that does exactly this?