The purpose of this example is to introduce 2-point spatial correlations and how they are computed, using PyMKS.
The example starts with some introductory information about spatial correlations. PyMKS is used to compute both the periodic and non-periodic 2-point spatial correlations (also referred to as 2-point statistics or autocorrelations and crosscorrelations) for a checkerboard microstructure. This is a relatively simple example that allows an easy discussion of how the spatial correlations capture the main features seen in the original microstructure. If you would like more technical details about 2-point statistics please see the theory section.
In [1]:
import pymks
%matplotlib inline
%load_ext autoreload
%autoreload 2
import numpy as np
import matplotlib.pyplot as plt
Let's first start with making a microstructure that looks like a 8 x 8 checkerboard. Although this type of microstructure may not resemble a physical system, it provides solutions that give some intuitive understanding of 2-point statistics.
We can create a checkerboard microstructure using make_checkerboard_microstructure function from pymks.datasets.
In [2]:
from pymks.datasets import make_checkerboard_microstructure
X = make_checkerboard_microstructure(square_size=21, n_squares=8)
Now let's take a look at how the microstructure looks.
In [3]:
from pymks.tools import draw_microstructures
draw_microstructures(X)
print X.shape
Now that we have created a microstructure to work with, we can start computing the 2-point statistics. Let's start by looking at the periodic autocorrelations of the microstructure and then compute the periodic crosscorrelation. This can be done using the autocorrelate and crosscorrelate functions from pymks.states, and using the keyword argument periodic_axes to specify the axes that are periodic.
In order to compute 2-pont statistics, we need to select a basis to generate the microstructure function X_ from the microstructure X. Because we only have values of 0 or 1 in our microstructure we will using the PrimitiveBasis with n_states equal to 2.
In [4]:
from pymks.stats import autocorrelate
from pymks import PrimitiveBasis
p_basis = PrimitiveBasis(n_states=2)
X_auto = autocorrelate(X, p_basis, periodic_axes=(0, 1))
We have now computed the autocorrelations.
Let's take a look at them using draw_autocorrelations from pymks.tools.
In [5]:
from pymks.tools import draw_autocorrelations
correlations = [('black', 'black'), ('white', 'white')]
draw_autocorrelations(X_auto[0], autocorrelations=correlations)
Notice that for this checkerboard microstructure, the autocorrelation for these 2 local states in the exact same. We have just computed the periodic autocorrelations for a perfectly periodic microstructure with equal volume fractions. In general this is not the case and the autocorrelations will be different, as we will see later in this example.
As mentioned in the introduction, because we using an indicator basis and the we have eigen microstructure functions (values are either 0 or 1), the (0, 0) vector equals the volume fraction.
Let's double check that both the phases have a volume fraction of 0.5.
In [6]:
center = (X_auto.shape[1] + 1) / 2
print 'Volume fraction of black phase', X_auto[0, center, center, 0]
print 'Volume fraction of white phase', X_auto[0, center, center, 1]
We can compute the cross-correlation of the microstructure function, using the crosscorrelate function from pymks.stats
In [7]:
from pymks.stats import crosscorrelate
X_cross = crosscorrelate(X, p_basis, periodic_axes=(0, 1))
Let's take a look at the cross correlation using draw_crosscorrelations from pymks.tools.
In [8]:
from pymks.tools import draw_crosscorrelations
correlations = [('black', 'white')]
draw_crosscorrelations(X_cross[0], crosscorrelations=correlations)
Notice that the crosscorrelation is the exact opposite of the 2 autocorrelations. The (0, 0) vector has a value of 0. This statistic reflects the probablity of 2 phases having the same location. In our microstructure, this probability is zero, as we have not allowed the two phases (colored black and white) to co-exist in the same spatial voxel.
Let's check that it is zero.
In [9]:
print 'Center value', X_cross[0, center, center, 0]
We will now compute the non-periodic 2-point statistics for our microstructure. This time, rather than using the autocorrelate and crosscorrelate functions, we will use the correlate function from pymks.stats. The correlate function computes all of the autocorrelations and crosscorrelations at the same time. We will compute the non-periodic statistics by omitting the keyword argument periodic_axes.
In [10]:
from pymks.stats import correlate
X_corr = correlate(X, p_basis)
All or some of the correlations can be viewed, using the draw_correlations function from pymks.tools. In this example we will look at all of them.
In [11]:
from pymks.tools import draw_correlations
correlations = [('black', 'black'), ('white', 'white'), ('black', 'white')]
draw_correlations(X_corr[0].real, correlations=correlations)
Notice that the maximum values for the autocorrelations are higher than 0.5. We can still show that the centers or the (0, 0) vectors are still equal to the volume fractions.
In [12]:
print 'Volume fraction of black phase', X_corr[0, center, center, 0]
print 'Volume fraction of white phase', X_corr[0, center, center, 1]
The non-periodic statistics are different from the periodic 2-point statistics along the diagonal vectors, but in both cases the probability of (0, 0) vector is still the volume fraction.
[1] S.R. Niezgoda, D.T. Fullwood, S.R. Kalidindi, Delineation of the Space of 2-Point Correlations in a Composite Material System, Acta Materialia, 56, 18, 2008, 5285–5292 doi:10.1016/j.actamat.2008.07.005
[2] S.R. Niezgoda, D.M. Turner, D.T. Fullwood, S.R. Kalidindi, Optimized Structure Based Representative Volume Element Sets Reflecting the Ensemble-Averaged 2-Point Statistics, 58, 13, 2010, 4432–4445 doi:10.1016/j.actamat.2010.04.041
[3] D.T. Fullwood, S.R. Kalidindi, and B.L. Adams, Second - Order Microstructure Sensitive Design Using 2-Point Spatial Correlations, Chapter 12 in Electron Backscatter Diffraction in Materials Science , 2nd Edition , Eds. A. Schwartz, M. Kumar, B. Adams, D. Field, Springer, NY, 2009.