Package: ilap
ilap: Python Tools for Numerical Inversion of the Laplace TransformOverviewTheilappackage implements the Fixed Talbot method for numerical inversion of the Laplace transform outlined by Abate and Valko (2004). Implementation is from scratch, based on the mathematical derivation presented in the paper.Two functions are exposed, both of which implement the same functionality, but each using a different backend.invert(lt,t)takes the name,lt, of some function of a single variable,lt(s),  defining a Laplace transform with Laplace variables, and a specified scalar (integer or float),t, representing the time at which the transform is to be inverted. It returns a float, representing the approximate value of the inverse transform at timet. The implementation uses Numpy or pure Python for all its numerics, and should accept essentially any functionlt, regardless of the libraries used in its definition.invert_mp(lt,t)operates the same way asinvert(lt,t), but it uses the mpmath arbitrary-precision library for its numerics. Because the numerical inversion of the Laplace transform is an ill-conditioned inverse problem, it is often necessary to use more than double precision to obtain useful results, and I recommend using this version if possible. The disadvantage of this method is that the mpmath library cannot work gracefully with Numpy/Scipy/Python math module functions: the transformltmustbe defined using only math functions defined in the mpmath module (most functions you could want are available), and basic Python arithmetic operations.invert_mpuses the currently set decimal precision of the mpmath module, which can be adjusted as needed before making a call toinvert_mp. See thempmath documentationfor more details.Usage ExampleThis example demonstrates numerical inversion of a Laplace-domain analytical solution to the advection-dispersion equation using both inversion methods, and comparing the results with a time-domain analytical solution:from ilap import invert, invert_mp
from matplotlib.pyplot import plot, legend, show, title, xlabel, ylabel
import mpmath as mpm
import numpy as np
from numpy import fromiter, float64, linspace, vectorize

#DEFINE LAPLACE TRANSFORMS FOR ADE AND TARGET SOLUTION
def L(alpha, d, v):
    return d**2/(2*alpha*v)

def M(d, v):
    return d/v 

#Laplace transform using numpy functions
def phi_trans(s, d, alpha, v): 
    def ig_trans(s, L, M):
        return np.exp(L/M - np.sqrt(L/M**2+ 2*s)/np.sqrt(1/L))
    return ig_trans(s, L(alpha, d, v), M(d, v))

#Laplace transform using mpmath functions
def phi_trans_mp(s, d, alpha, v): 
    def ig_trans(s, L, M):
        return mpm.exp(L/M - mpm.sqrt(L/M**2+ 2*s)/mpm.sqrt(1/L))
    return ig_trans(s, L(alpha, d, v), M(d, v))

#Target analytic solution
def phi_direct(t, d, alpha, v): 
    def ig_direct(t, L, M):
        return np.sqrt(L/(2*np.pi*t**3))*np.exp(-L*(t-M)**2/(2*M**2*t))
    return ig_direct(t, L(alpha, d, v), M(d, v))

#PHYSICAL PARAMETERS
d = 1.5         #distance [m]
alpha = 3e-2    #dispersivity [m]
v = 0.53e-3     #velocity [m/s]
v_t = linspace(1, 7000, num=100) #times [s]

#PLOTTING
#Plot target solution
df = vectorize(lambda t: phi_direct(t, d, alpha, v))
v_PDF = df(v_t)
plot(v_t, v_PDF, 'ks', markerfacecolor='none', ms=6, markeredgecolor='darkolivegreen', label="Exact solution")

#Plot numerical inversion via invert()
lt = lambda s: phi_trans(s, d, alpha, v)
v_PDFt = fromiter(map(lambda t: invert(lt,t), v_t), dtype=float64)
plot(v_t, v_PDFt, lw=2, color="navy", label="Solution via invert()")

#Plot numerical inversion
lt = lambda s: phi_trans_mp(s, d, alpha, v)
v_PDFt = fromiter(map(lambda t: invert_mp(lt,t), v_t), dtype=float64)
plot(v_t, v_PDFt, ls=(0, (3, 3)), lw=2, color="goldenrod", label="Solution via invert_mp()")

#Format the plot area
xlabel("Time")
ylabel("Probability density")
title("Test of ilap module inversion methods on ADE solution")
legend()
show()ReferenceAbate, J. and P. P. Valko, 2004. Multi-precision Laplace transform inversion.International Journal for Numerical
Methods in Engineering, 60(5), 979. doi:10.1002/nme.995.