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Pieter Barendrecht
@pjbarendrecht
Thanks! Using P.all_roots() still produces an error when doing so (NotImplementedError: sorted roots not supported over ZZ[log(2)]), but roots(P) works just fine
Kunal Mahatha
@kunal-mahatha
Hey everyone,
I am Kunal. I want to contribute to sympy, but I am a beginner and I know basic to intermediate Python. Could someone please guide me on how the contribution procedure works here, and suggest to me some good beginner-friendly issues to start working on?
Taven
@daegontaven
hi, i'm an amateur at logic, and was wondering if it was possible to generate latex semantic tableaux trees using sympy?
Joao Aguirre
@aguirreeng
Hello everyone, just a simple question (I hope), is it possible to do nested summations with dependent indexes using the Concrete class Sum, replicating in a "single command" things like
f(x)=i=03(j=i+14axiyj) f \left ( {x} \right ) = \sum_{i = 0}^{3} {\left ( {\sum_{j = i + 1}^{4} {\frac{a}{x_{i} - y_{j}}}} \right )}
1 reply
Brandon Feder
@brandon-feder
Hey guys. I was just wondering if anyone knows what algorithm is being used in the GeneralSumOfSquaresclass used here. Is there a paper I can reference/explanation, etc?
Aaron Meurer
@asmeurer
@brandon-feder there are some links in the source, e.g., in the power_representation function. Otherwise you might find some references in some of the old 2013 posts in this blog https://thilinaatsympy.wordpress.com/
Jason Ross
@Jason-S-Ross

I'm having trouble learning the diffgeom module. I'm trying to compute covariant derivatives in spherical coordinates and I feel like I'm missing something.

Here's what I'm working with:

from sympy import *
from sympy.abc import x, y, z, r, theta, phi
from sympy.diffgeom import CoordSystem, Manifold, Patch, TensorProduct as TP

R3 = Manifold("R3", 3)
S = Patch("S", R3)
relations = {
    ("Car3D", "Sph") : Lambda(
        (x, y, z),
        Matrix([
            sqrt(x**2 + y**2 + z**2), 
            acos(z / sqrt(x**2 + y**2 + z**2)),
            atan2(y, x),
        ])
    ),
    ("Sph", "Car3D"): Lambda(
        (r, theta, phi),
        Matrix([r * sin(theta) * cos(phi), r * sin(theta) * sin(phi), r * cos(theta)])
    )
}
Car3D = CoordSystem("Car3D", S, [x, y, z], relations)
Sph = CoordSystem("Sph", S, [r, theta, phi], relations)

I can compute the metric tensor in spherical coordinates by doing the following:

g = (Car3D.jacobian(Sph) @ Car3D.jacobian(Sph).T).simplify()

However, this computes the metric tensor with respect to $x, y, z$, while I'd like to write the metric tensor with respect to $r, \theta, \phi$:
[10001x2+y2+z20001x2+y2]\left[\begin{matrix}1 & 0 & 0\\0 & \frac{1}{x^{2} + y^{2} + z^{2}} & 0\\0 & 0 & \frac{1}{x^{2} + y^{2}}\end{matrix}\right]
I can do a substitution, but it's kind of awkward:

x, y, z = Car3D.symbols
r, theta, phi = Sph.symbols
forward_subs = {
    x: r * sin(theta) * cos(phi),
    y: r * sin(theta) * sin(phi),
    z: r * cos(theta)
}
g_sph = g.subs(forward_subs).simplify()

[10001r20001r2sin2(θ)]\left[\begin{matrix}1 & 0 & 0\\0 & \frac{1}{r^{2}} & 0\\0 & 0 & \frac{1}{r^{2} \sin^{2}{\left(\theta \right)}}\end{matrix}\right]
This gives me the expected metric tensor as a matrix but there's a lot of extra effort:

  • I have to define the forward and backward transformations BEFORE I declare forward_subs since the CoordinateSymbol "x" does not exist until I create Car3D, and I have to provide the forward and backward transformations to create Car3D.
  • Converting from one coordinate system to another uses a dictionary that duplicates all the information already defined in the coordinate systems
  • Computing a metric tensor by taking the Jacobian times its transpose seems like extra effort
  • I still haven't got a tensor expression for the metric tensor

I can convert the metric tensor Matrix to a tensor expression as follows:

g_sph_tens = 0
for i, e_i in enumerate(Car3D.base_oneforms()):
    for j, e_j in enumerate(Car3D.base_oneforms()):
        g_sph_tens += g_sph[i, j] * TP(e_i, e_j)

However, computing the Christoffel symbol for g_sph_tens using metric_to_Christoffel_2nd gives all zeros, which is incorrect.

Can somebody help me out with this? It seems like I'm missing some fundamentals.

1 reply
Matías Senger
@SengerM

Hi, I want to learn SymPy to do some calculations. I am practicing with the electromagnetic Lagrangian term $F_{\mu\nu}F^{\mu\nu}$. I have defined $F$ in the way that is explained in the documentation but cannot figure out how to go from there to $E^2 + B^2$. How am I supposed to do this?

Up to now I have this:

Ex, Ey, Ez, Bx, By, Bz = sp.symbols('E_x E_y E_z B_x B_y B_z')
c = sp.symbols('c', positive=True)

F = spT.TensorHead('F', [Lorentz, Lorentz], spT.TensorSymmetry.fully_symmetric(-2))

repl = {Lorentz: sp.diag(1, -1, -1, -1)}
repl.update({F(-mu,-nu): [
    [0, Ex/c, Ey/c, Ez/c],
    [-Ex/c, 0, -Bz, By],
    [-Ey/c, Bz, 0, -Bx],
    [-Ez/c, -By, Bx, 0]]}
)

and I have tried (F(mu,nu)*F(-mu,-nu)).replace_with_arrays(repl, [mu,nu]) and also F(mu,nu).replace_with_arrays(repl, [mu,nu])*F(-mu,-nu).replace_with_arrays(repl, [mu,nu]).

6 replies
Priyanshu Agarwal
@priyanshuone6
Hey, I have some huge equations but they are getting printed incomplete and half when I use sympy preview for pdf (see the pdf here) , could you please help me with this
sympy.preview(expr, output="pdf", viewer="file", filename="DFN_equations.pdf", dvioptions=['-D', '1100'], euler=False)
Jason Ross
@Jason-S-Ross

I wanted to expand on my question from earlier since it may be too specific.
I am working through some equations from the theory of elasticity.

The differential equation I am trying to work with is the equation
for compatibility of small displacements in a strained isotropic elastic body.
This is written as
(12η)vijj+vjji=0(1 - 2\eta) v^i|^j_j + v^j|^i_j = 0
where
fijf^i|_j
represents the covariant derivative of f with respect to j, and
fijf^i|^j
represents the covariant derivative of f with respect to j
with the j index raised (this convention is from Green and Zerna -
I don't know if this is a standard notation).

We can use solutions of the above differential equation to compute
the stress tensor as follows:

τijμ=gjsvis+girvjr+2η12ηgijvrr\frac{\tau^{ij}}{\mu} = g^{js} v^i|_s + g^{ir} v^j|_r + \frac{2 \eta}{1 - 2 \eta} g^{ij} v^r|_r

One of the solutions to the displacement equation is as follows:

vi=Fiv_i = F|_i

where F is a harmonic function.

What's a good way to

  1. Verify that this satisfies the displacement equation
  2. Plug this into the stress tensor equation and display the result in Cartesian
    and spherical coordinates?
Megan Ly
@meganly
Is there a way to get Sympy to pull a constant inside of an integral without evaluating it? For example, rewriting c*Integral(f(x), (x,a,b)) as Integral(c*f(x), (x,a,b)). I'm struggling to get replace to work.
4 replies
Ruturaj57
@Ruturaj57
Hello everyone!
Am Ruturaj, computer science student.
I want to contribute to this open source, so can anyone guide me please?
Cherish Sachdeva
@csachdeva83
Hello Everyone!
Hope you all are having a nice day.I want to integrate(cos(3theta)/(5-4cos(theta)),(theta,0,2pi)) this expression whose
answer is pi/12 but sympy does not executes the integral. So,I replaced cos(3
theta) with
4cos(theta)*3-3cos(theta) then I am obtaining -21pi/8.Also when I replaced cos(3theta) with
cos(theta) sympy executed the integral and gave -pi/2.Can anyone please elaborate why sympy is not executing
cos(3*theta) in integral?
Kalevi Suominen
@jksuom
Integrals of that type should be handled by the risch integrator but that part of the algorithm has not been implemented (yet). Currently, heurisch will be used as a fall-back integrator but it looks like there is a bug that leads to a wrong result.
Megan Ly
@meganly
Is there a way to get the Latex printer to print Integral(x**2,(x,1,2)) as the string '\\int_{1}^{2} x^{2}\\, dx' instead of '\\int\\limits_{1}^{2} x^{2}\\, dx'?
Aaron Meurer
@asmeurer
@meganly apparently latex(mode='inline') does that.
I wonder what the point of \limits is.
12x2dx\int_1^2 x^2\, dx vs. 12x2dx\int\limits_1^2 x^2\, dx
I guess \limits puts them directly above or below the integral sign. That does seem better for non-inline mode, especially if the limits can be long.
then again the non-limits version does look better even for equation mode when the limits are small. Maybe there should be some heuristics here.
Aaron Meurer
@asmeurer
I opened sympy/sympy#21851 for this.
Megan Ly
@meganly
Thanks. My reason for not wanting \limits is that the \limits command is not supported by MathQuill which causes issues for rendering Latex in a web browser.
ThePauliPrinciple
@ThePauliPrinciple
hey hey, I saw in the release notes that ArraySymbol was added, however, I couldn't find the documentation on it, does anyone have any hints where to find more information?
Aaron Meurer
@asmeurer
It looks like it isn't documented very much yet. You may have to take a look at the PR that added it for now to get some more information.
ThePauliPrinciple
@ThePauliPrinciple
Thanks, I looked into the source and it basically is a way to conveniently get symbols with labes that make sense for arrays and array elements, but there is not other functionality that really requires documentation
Aaron Meurer
@asmeurer
I think it should be roughly the same idea as MatrixSymbol
Het
@hetp111
Any docs to build sympy from source?
2 replies
ThePauliPrinciple
@ThePauliPrinciple
Lambdify uses _EvaluatorPrinter and I want it to behave slightly differently. Is there any option other than a lot of code duplication/modifying the source? Specifically, I don't want it to use return, but instead I want to use ASTs return (so that I can e.g. go for multiple lines in one go or use control flow logic from AST)
ThePauliPrinciple
@ThePauliPrinciple
In particular, my solution would be to replace '''funcbody.append('return ({})'.format(self._exprrepr(expr)))''' with '''funcbody+=self._exprrepr(expr).splitlines()''' if expr is a CodeBlock on line 1092 of utilities/lambdify.py
also, gratz on the 1.9 release :D
pratham-saxena
@pratham-saxena
Heyy devs, i am new to open source and i would certainly love to help in whichever way possible. Is there anything i could help you guys with?
ThePauliPrinciple
@ThePauliPrinciple
ThePauliPrinciple
@ThePauliPrinciple
When I want to copy some file from sympy and modify it slightly for my own library, can I do that? I would guess I need to add the Sympy license to my own project? If so, do I need to add all the "external" licenses of the sympy project too, or only the main sympy license?
Jason Ross
@Jason-S-Ross
Is there a generalized Kronecker Delta in sympy?
https://en.wikipedia.org/wiki/Kronecker_delta#Generalizations
pratham-saxena
@pratham-saxena
@ThePauliPrinciple thanks for answering sir .
ThePauliPrinciple
@ThePauliPrinciple
There is a levi-civita symbol, which you may be able to use @Jason-S-Ross
alternatively, you could explicitly write the pxp determinant https://docs.sympy.org/latest/tutorial/matrices.html#determinant
Jason Ross
@Jason-S-Ross
@ThePauliPrinciple I think the levi-civita symbol would work. Good thinking
s3k
@s3k:matrix.org
[m]
Hi Folks! Is it possible to use sympy to obtain the probability density function of a transformed random variable?
kdsch
@kdsch:matrix.org
[m]
I am not expecting the results given by https://tinyurl.com/y2vzw6dp
Matías Senger
@SengerM

I am working in a simple QFT calculation and would like to do it using Sympy to learn (and also check my result). I have found the Quantum Mechanics module but cannot see how to start using it for my purpose. I have defined these quantities:

import sympy.physics.quantum as Q
vacuum = Q.OrthogonalKet(0)
annihilation_op = Q.Operator('a')
creation_op = Q.Dagger(annihilation_op)

and now I want to tell Sympy that an=nn1a |n\rangle = \sqrt{n} | n-1 \rangle if n>0n>0 else 00 and an=n+1n+1a^\dagger | n \rangle = \sqrt{n+1} | n+1 \rangle. How would I do this? Also, how do I impose the commutation relations between aa and aa^\dagger?

GayanathSamuditha
@GayanathSamuditha

Hi all,

I am just a new user for SymPy. I am self learning this library for my undergrauate research. But in the middle of the process I am stucked with one code.

So I have defined a function with a subscript.

                     U_n= x^n + 1/x^n

When I consider (U_1)^3 I get (substitute n=1)

                    (U_1)^3 = (x+1/x)^3

Then after simplifying this I get

                    (U_1)^3 = (x^3 + 1/x^3) + 3(x+ 1/x)      

But one can see this answer as

                                   (U_1)^3 =   U_3 + 3U_1

How to get the output in terms of U_n 's ?

Can someone please give an idea how to build this code using SymPy. It would be a very big help for my research.

Thank you very much.

Gayanath Chandrasena.

ThePauliPrinciple
@ThePauliPrinciple
You can use .subs to substitute x+1/x with U_1
But, you need a better definition of what you want
since U_1^3 is already in terms of U_n's?
treffenl
@treffenl:matrix.org
[m]
Cheers! I'm having an issue with an integration where sympy outputs a piecewise with the condition dr*(k-1) < dr*(k+1), which is obviously true, since dr = symbols('Delta',real=True,positive=True,nonzero=True) and k = symbols('k',integer=True,real=True), yet sympy doesn't seem to thing this is the case. Am I doing something wrong?

Also I get

In [54]: print(ask(dr*(k-1) < dr*(k+1)))
None

but

In [55]: print(ask(dr*k-dr < dr*k+dr))
True
1 reply