Integration Lab

Integration Lab#

In this lab, you will explore two important challenges in numerical integration:

  1. Handling improper integrals using coordinate transformation. Many real-world integrals have infinite limits or singularities. Direct numerical integration often fails, so we apply variable transformations to map the integral to a finite domain.

  2. Investigating convergence properties for functions with discontinuities. Standard numerical methods assume smoothness for high accuracy. If the function has a jump discontinuity, we will observe how the convergence rate deteriorates.

Handling an Improper Integral via Coordinate Transformation#

Consider the improper integral:

(171)#\[\begin{align} I = \int_0^{\infty} \frac{1}{1 + x^2} dx. \end{align}\]

This integral is well-known, and its exact value is:

(172)#\[\begin{align} I = \frac{\pi}{2}. \end{align}\]

However, standard numerical integration methods fail because the domain extends to infinity. To solve this, we introduce a coordinate transformation that maps the infinite domain \([0, \infty)\) to a finite domain \([0,1]\).

Coordinate Transformation#

A common transformation is:

(173)#\[\begin{align} x = \frac{t}{1 - t}, \quad \text{where } t \in [0,1]. \end{align}\]

Differentiating,

(174)#\[\begin{align} dx = \frac{dt}{(1 - t)^2}. \end{align}\]

Rewriting the integral in terms of \(t\):

(175)#\[\begin{align} I &= \int_0^1 \frac{1}{1 + \left(\frac{t}{1 - t}\right)^2} \frac{dt}{(1 - t)^2} \\ &= \int_0^1 \frac{dt}{(1-t)^2 + t^2} \\ &= \int_0^1 \frac{dt}{1 - 2t + 2t^2} \end{align}\]

This transforms the infinite limit \(x = \infty\) to the finite limit \(t = 1\), allowing us to apply numerical integration techniques.

import numpy as np
from matplotlib import pyplot as plt

# HANDSON: Define the original function
def f(x):
    pass

# HANDSON: Define the transformed function
def ft(t):
    pass

# HANDSON: Implement Middle Riemann Sum
def middle(f, N, a=0, b=1):
    pass

# Perform the integration using the transformed variable
N = 64  # Number of sub-intervals
I = np.pi / 2
I_middle = middle(ft, N)

# Print results
print(f"Middle Riemann Sum (N={N}): {I_middle}")
print(f"Exact Integral: {I}")
print(f"Absolute Error: {abs(I_middle - I)}")

Middle Riemann Sum (N=64): None
Exact Integral: 1.5707963267948966

---------------------------------------------------------------------------
TypeError                                 Traceback (most recent call last)
Cell In[5], line 9
      7 print(f"Middle Riemann Sum (N={N}): {I_middle}")
      8 print(f"Exact Integral: {I}")
----> 9 print(f"Absolute Error: {abs(I_middle - I)}")

TypeError: unsupported operand type(s) for -: 'NoneType' and 'float'

Integrating a Function with a Jump Discontinuity#

Many numerical integration methods assume smoothness of the function. However, when the function has a jump discontinuity, the convergence rate degrades significantly.

Consider the function:

(176)#\[\begin{align} f(x) = \sin(\pi x) + \begin{cases} 0, & 0 \leq x < 0.5 \\ 1, & 0.5 \leq x \leq 1 \end{cases} \end{align}\]

We compute the definite integral:

(177)#\[\begin{align} I = \int_0^1 f(x) dx. \end{align}\]

Since the function is piecewise constant, the exact integral is \(2/\pi + 1/2\). However, standard numerical integration methods will struggle to approximate this accurately due to the jump at \(x = 0.5\).

# HANDSON: Define the left and right functions
def fL(x):
    pass

def fR(x):
    pass

def f(x):
    return np.where(x < 0.5, fL(x), fR(x))

# HANDSON: Implement the Trapezoidal Rule
def trapezoidal(f, N=8, a=0, b=1):
    pass

# HANDSON: Implement Simpson's Rule
def simpson(f, N=8, a=0, b=1):
    pass

# Compute exact integral
I = 2/np.pi + 0.5

# Compare convergence for different methods
Ns = [4, 8, 16, 32, 64, 128, 256]
errs_trap  = []
errs_simp  = []
errs_trap2 = []
errs_simp2 = []

for N in Ns:
    I_trap  = trapezoidal(f, N)
    I_simp  = simpson    (f, N)
    I_trap2 = trapezoidal(fL, N//2, 0, 0.5) + trapezoidal(fR, N//2, 0.5, 1)
    I_simp2 = simpson    (fL, N//2, 0, 0.5) + simpson    (fR, N//2, 0.5, 1)
    errs_trap .append(abs(I_trap  - I))
    errs_simp .append(abs(I_simp  - I))
    errs_trap2.append(abs(I_trap2 - I))
    errs_simp2.append(abs(I_simp2 - I))

# Plot error convergence
plt.loglog(Ns, errs_trap,  'o--', label='Trapezoidal Rule')
plt.loglog(Ns, errs_simp,  's--', label='Simpson’s Rule')
plt.loglog(Ns, errs_trap2, 'o-',  label='Trapezoidal Rule 2')
plt.loglog(Ns, errs_simp2, 's-',  label='Simpson’s Rule 2')
plt.loglog(Ns, np.array(Ns)**(-1.), ':', label=r'$N^{-1}$ reference')
plt.loglog(Ns, np.array(Ns)**(-2.), ':', label=r'$N^{-2}$ reference')
plt.xlabel('Number of Intervals (N)')
plt.ylabel('Absolute Error')
plt.legend()
plt.title('Convergence of Numerical Integration on a Discontinuous Function')
plt.show()

Observations

  1. Degraded Convergence Rate

    • For smooth functions, Simpson’s rule is expected to converge at \(\mathcal{O}(N^{-4})\).

    • However, due to the discontinuity at \(x = 0.5\), it instead converges at \(\mathcal{O}(N^{-1})\).

  2. Poor Accuracy for Large (N)

    • Increasing (N) does not always help significantly because the integration points do not align with the discontinuity.

  3. Potential Fixes

    • Refinement Near the Discontinuity: Placing additional points near \(x = 0.5\) (which we didn’t implement).

    • Splitting the Integral: Compute separate integrals for \([0, 0.5]\) and \([0.5, 1]\).

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