25. The Centre Cannot Hold II: Elliptic Fourier Analysis
Written by Norm MacLeod - The Natural History Museum, London, UK (email: email@example.com). This article first appeared in the Nº 79 edition of Palaeontology Newletter.
Although I’ve never seen it acknowledged in any description of the EFA method, there is quite a suspicious similarity between EFA and ZR-based Fourier analysis that has always struck me as being suggestive of a conceptual link. In order to illustrate this let’s return to the pathological outline of the benthic foraminiferal species Ramulina globulifera (Fig. 1).
Figure 1. Shape of the spinose benthic foraminifer species Ramulina globulifera. A. Image of R. globulifera specimen, B. implied outline defined by an interpolation of 300 equally spaced boundary outline semilandmarks. The starting point for digitization is shown by the green landmark.
TAs you will recall from the last column, the problem with this outline is that it’s very far from exhibiting a single-valued character. No matter what center is selected the outline cannot be represented accurately by a shape function based on the lengths of radius vectors drawn from the center to the periphery such that the angle between the radius vectors is constant and all radius vectors cross the outline at one, and only one, point. The ZR shape function solves this problem by interpolating a set of semilandmark points around the outline such that the inter-point distance is constant and the shape represented by a series of net angular deviations from a starting segment. This operation transforms the outline of any curve, no matter how complex, into a pattern that conforms to the definition of a mathematical function (Fig. 2).2
Figure 2. Zahn and Roskies shape function for a 300-point interpolation of the R. globulifera outline semilandmark data expressed as the net deviation of angles drawn between successive semilandmark around the form (ϕ).
The Z-R technique transforms a complicated outline into an alternative format that loses none of the outline’s geometric information content, but is tractable to handle in the context of a Fourier analysis. It works fine. But this isn’t the only solution to complex outline representation.
Note that the abscissa (traditionally the ‘x-axis’) of the plot in Figure 2 is simply the ordinal number of intervals round the the outline. There are n such intervals in any curve where n is the number of semilandmarks used to represent the curve’s form or shape. Obviously the ZR shape function is employing variations in the coordinate positions of both the x and y axes in order to determine the next angular direction to subsequent boundary outline locations (ϕ). But what if we considered these x and y deviations between successive semilandmark locations separately?
Figure 3 shows the form functions that result from plotting the x coordinates and the y coordinates of successive semilandmark points separately.
Figure 3. Form functions for separate x (A) and y (B) coordinate values of the R. globulifera outline.
These are form functions rather than shape functions because, as the raw coordinate values were used, the x and y values retain their scale. Since only one form is shown here the distinction between form and shape is not important. Regardless, it should be noted that, since this representation can utilize the raw coordinate values, it is possible to use this shape function to perform a form analysis or, if the semilandmark points are rescaled to eliminate size differences among a set of outlines, a shape analysis.
Like the ZR shape function, all the geometric information present in the original semilandmark coordinate data is present in these plots. Also as with the Z-R shape function, the advantage of this format is that the resulting data conform to the definition of mathematical functions, and so can be subject to methods of analysis designed to extract information from function-type datasets. This will always be the case for any conceivable outline; even open outlines and/or those that intersect themselves. Moreover, because these shape/form functions are simply direct readings of variation in the x and y aspects of the outline boundary coordinates, the constraint of equi-angularity (standard radial Fourier analysis) or equal inter-coordinate spacing (ZR Fourier analysis) is relaxed. Forms can be represented by any number of semilandmark coordinate points the analyst deems appropriate and inter-landmark spacings can assume any value(s) necessary to ensure comparable portions of the outline are aligned properly in the semilandmark sequences. The only requirements are that the same number of semilandmarks be used to represent the form/shape of the outlines of all specimens in the sample and (for EFA) that all outlines in the sample be closed (= end at the same landmark coordinate position at which they began). In practice, the ability to vary the inter-semilandmark spacing as a strategy for ensuring biological correspondence between outline segments has rarely been used in any EFA application. But this does not mean it could not be used to boost biologically important signals in the data and improve the interpretability of EFA results.
If an alternative form of outline shape/form function representation was all that was involved with an EFA it would simply represent a minor variant of the ZR shape function approach. However, the developers of this method went further than Zahn and Roskies (1971) and used the separation of x and y form/shape functions as the beginning of a new approach to the Fourier analysis of closed-form outlines. Their key insight in this regard was to think of the total set of length and orientation steps around any outline (t) as being the sum of apparent displacements in x and y directions (see Kuhl and Giardina 1982, Ferson et al. 1985, Lestrel 1997).
This allowed Kuhl and Giardina (1982) to derived a set of parametric equations that could be used to fit a set of Fourier harmonic amplitudes to the outline semilandmark data directly. The elliptic Fourier coefficients for the x aspect of the form/shape function are:
Similarly, the elliptic Fourier coefficients for the y aspect of the form/shape function are:
Giardina and Kuhl (1977) showed that equations 25.1 and 25.1 specify an outline-specific series of elliptical shapes of monotonically increasing spatial detail that, when summed together, represent an approximation of the form. This approximation minimizes of the deviation of the empirical outline with respect to the estimated model in a least-squares sense. The EFA outline estimation process can be illustrated by reconstructing the form of the R. globulifera outline using different numbers of EFA harmonics (Table 1). All harmonics calculated in this manner are independent from each other. Therefore, the sets of harmonic coefficients representing each can be used as empirical form-descriptors in their own right, either singly or in combination.
Table 1. Sequential reconstruction of the R. globulifera form from the four elliptic Fourier terms calculated over different sets of harmonic amplitudes (n).
Mistakes are often made by inexperienced EFA practitioners (indeed by inexperienced outline data analysts in general), by using arbitrary criteria to decide how many Fourier harmonics to use to quantify the shapes present in a sample. This is especially important in the context of EFA analysis because four terms are required to quantify each harmonic: two terms for the x series and two for the y. If reduction of the dimensionality of a shape representation problem is the purpose of undertaking an EFA, the most accurate representation of the R. globulifera outline presented in Table 4 (n = 40) would require 160 terms to represent. While this is a distinct improvement over the 300 x,y coordinates used to quantify the outline of the original shape, it remains a high-dimensional dataset. However, if the number of harmonics used to represent this form was cut back to a lower number — say 10 — in order to achieve substantial dimensionality reduction (from 600 variables to 40), the quality of the form’s representation would suffer. Of course, the R. globulifera outline is an extreme example. In many cases relatively small numbers of harmonics will be able to represent biological forms of interest (see Ferson et al. 1985 for an example). Nevertheless, it is always advisable to make this critical decision on the basis of an inspection of reconstructed forms rather than simply plucking a value for N out of thin air.
In addition to containing information about the shape of an an outline, the An, Bn, Cn, and Dn coefficients contain information about the location, size, and rotational orientation of the outline. In some cases this information may be of interest. But in most biological morphometric analyses shape variation is the primary target. Although these extraneous variables could always be corrected for through various ad hoc normalization procedures or by subjecting the semilandmark sets to generalized least-squares Procrustes alignment (see Rohlf and Slice 1990, MacLeod 2009a) prior to EFA, Kuhl and Giardina (1982) specified a direct procedure for normalizing the EFA coefficients calculated from raw outlines for these factors. The basic equation for achieving this normalization is as follows.
Obviously several of the terms of this expression need to be explained and defined. The E* coefficient is the magnitude of the best fitting ellipse. This is, what Kuhl and Giardina (1982) regarded as, effectively, the size term, the influence of which is removed from the data by reciprocal scaling. This E* coefficient is calculated using the following expressions.
Of course, the A1, B1, C1, and D1 terms in equations 25.9 and 25.10 are the four coefficients associated with the first EFA harmonic which is, in all cases, an ellipse (see Table 1). The ϴ term is the angle between the starting point of the outline digitization sequence and the major axis of the ellipse. This angle is given by the following expression.
The ϴ correction is factor is used in equations 25.7, 25.9, and 25.10 to align the EFA harmonic sequence to an internal standard set by the first harmonic. The final set of EFA coefficients are adjusted to bring the estimated outline model into a standing rotational orientation via calculation of the ϕ coefficient, as follows.
When these normalizations are applied the values of a1 = 1.0 and those and b1 and c1 = 0.0 signalling the loss of information inherent in the normalization procedure. This procedure is formally equivalent to the normalizations applied by Procrustes superposition. A comparison of the raw and normalized EFA coefficients for the first ten EFA harmonic amplitudes for the R. globulifera outline is shown in Figure 4.
Figure 4. Raw (A) and normalized (B) EFA coefficients for the first 10 EFA harmonic amplitudes of the R. globulifera outline. Note rescaling of all harmonic spectra as well as the setting of a1 to 1.0 and both b1 and c1 to 0.0 as a result of the normalization procedure.
While most applications of EFA in morphometric contexts will require implementation of all three normalizations, there may be occasions in which size, location of the starting point for digitization, and/or rotation are parameters of interest. In these cases the form of equation 25.7 can be adjusted so that one or more of these factors remains present in the harmonic spectra.
Once a set of normalized harmonic spectra have been obtained from a sample of shapes these are most typically used as input into a secondary multivariate data analysis procedure (e.g., PCA, PCoord, MDS, CVA, PLS) in order to extract the major dimensions of shape variation, represent patterns of shape variation in a low-dimensional ordination space, investigate questions of group separation or distinctiveness, and/or document the association of particular aspects of outline shape variation with variables external to the morphological data per se and, in so doing, test causal hypotheses. As I have noted in previous discussions of these procedures, results generated by their application can be inspected and/or used as input into tertiary statistical procedures designed to test specific patterns via reference to a probability or likelihood models. They can also be used to obtain models of shape variation patterns at particular points along the axes of the ordination spaces so defined, or along any trajectory through the hyper-dimensional ordination space that the data analyst cares to specify.
As an example of the use of EFA in the context of a morphometric investigation I will apply it to the same benthic foraminiferal test outlines I used in the last column to illustrate use of the ZR shape function with standard Fourier analysis. The images from which these outlines were derived are shown in Figure 5.
Figure 5. Benthic foraminiferal shapes used in the example analysis. Note the presence of shapes with multi-valued outlines.
Each outline was quantified using 200 equally-spaced semilandmark points with the landmark from which digitization started being located at the center of the aperture. Inspection of outline morphologies reconstructed using different numbers of EFA harmonic amplitudes indicated that, for this dataset, the major features of each outline could be captured using the first 25 normalized elliptic Fourier harmonics (see Table 2).
Table 2. Outline silhouettes for benthic foraminiferan shapes reconstructed from normalized EFA coefficients using 25 harmonic amplitudes. See Figure 4 for species names.
Figure 6. Distribution of the 12 benthic foraminiferan test outlines shown in Figure 5 and Table 2 in the shape space formed by the first three principal components of the covariance matrix calculated between normalized EFA coefficients. See text for discussion.
Inspection of the distribution of species along these three principal component axes suggests that PC-1 captures the distinction between tests characterized by uniserially arranged globular chambers (e.g., Hormosinelloides guttifer) and flaring tests with multi-serially arranged chambers (e.g., Bulimina mexicana), PC-2 the distinction between tests whose chambers increase in size with development (e.g., Hormosinelloides guttifer) as opposed to those whose tests are characterized by a relatively thin, tubular neck (e.g., Lituotuba lituiformis), and PC-3 the distinction between tests with complex, lobulate peripheries that are thick in the middle (e.g., Uvigerina proboscidea) relative to those characterized by a medial constriction (e.g., Reophanus berggreni). It’s also important to note that, in terms of outline shape variation, for this sample Lagena sulcata, Lituotuba lituiformis, and Reophanus berggreni all represent shape outliers.
While sufficient for a interpretation of the generalized geometry of the principal component spaces, the qualitative trends described above fail to represent the detailed geometric contrasts that exist along the primary PCA vectors, information which has been captured by the original outline data and employed by the eigenvector equations that define PC-1, PC-2, and PC-3. Fortunately, we are not restricted to such qualitative approaches to EFA shape space interpretation.
The eigenvector loading coefficients that define PC-1, PC-2 and PC-3 represent a series of cosines that quantify the angular relationship between these eigenvectors and the original variables in a manner that takes note of covariance structure of these data (see MacLeod 2005). Since this is the same information we used previously to construct geometric modes of PCA form/shape spaces for landmark (MacLeod 2009b, 2010a) and outline data (MacLeod 2011), it should be possible to create similar models for the EFA-defined PCA ordination spaces shown in Figure 4. It’s possible to calculate these models using either the direct landmark or thin plate spine approaches (see MacLeod 2009b and 2010a respectively), though the former seems the more natural and informative choice for these data. The models calculated by this method will be expressed in terms of the original variables submitted to the EFA-PCA analysis. These may be converted back to sets of x,y coordinate data using the following equations.
Application of equations 25.13 and 25.14 to sets of EFA amplitude coefficients calculates at a series of coordinate point locations along the PC-1, PC-2 and PC-3 axes resulted in construction of the along-axis shape models shown in Table 3.
As can be seen graphically in the table — especially when the individual along-axis shape models are overlain to create a ‘strobe‘ effect — the geometric trend being expressed along each axis is a function of (1) the degree of inflation (PC-1) and lobateness PCs 2 & 3) of the test peripheries on either side of the test’s long axis. Based on these results the distinction between low scores and high scores along PC-1 reflects the distinction between broadly elliptical shapes with concave to convex lateral margins respectively. The PC-2 axis captures aspects of spatial changes in lateral lobateness with respect to the test’s long axis, with low scores representing lobe formation confined to late stages of test development and high scores representing patterns of lateral lobe formation that occur at earlier developmental stages. Finally, PC-3 expresses distinctions between the lobateness of the medial portion of the test with respect to the two ends. Here, tests characterized by strongly convex medial outlines sandwiched between distinctly pinched terminal regions project to low positions along this axes while those characterized by bulbous terminal regions separated by a narrow, concave, medial lobe project to high positions. The dramatic increase in geometric insight into the natural of EFA ordination spaces that can be achieving through use of models to query and interpret the EFA-PCA is (I hope) obvious.
Like Z-R Fourier analysis, elliptic Fourier analysis effectively addresses the need for a numerical method that can be used to represent outline form/shape variation in a rigorously quantifiable, geometric manner while overcoming the limitations of radial Fourier analysis in terms of its ability to treat single and multivalued outlines and its freedom from being subject to the centroid-location problems which plague the latter, at least with respect to some outlines. Elliptic Fourier analysis is fully extensible to the treatment of 3D outlines (see Lestrel 1997). Owing to its dependence on ellipses EFA is technically restricted to the analysis of closed outlines. However, Kuhl and Giardina (1982) include example analysis of forms that come very close to being open curves in their discussion of EFA applications, though the ability of EFA to reconstruct such curves seems decidedly suboptimal to me.
Owing to the availability of public-domain software for performing EFA, the technique has proven reasonably popular with morphometricians despite the fact that much of the early geometric morphometric literature was rather hostile to outline analysis methods in general and Fourier-based methods in particular. There were two reasons for this. The first has to do with non-correspondence between the biological features that sequences of semi-landmark points may fall on when an outline is sampled. This is a well-known problem that I’ll have more to say about in my discussion of eigenshape analysis. In terms of sampling the form, EFA can circumvent this issue rather easily because it does not assume that the spacing between semi-landmark points will be equal. Accordingly, it is a relatively simple matter to subdivide the outline into segments at true landmarks and use semi-landmark sequences to ‘join’ the landmarks in a matter that accurately represents for form/shape of of the inter-landmark boundary curves (see MacLeod 1999 for an example of this procedure). Data collected in this way can be submitted to an EFA analysis without any further processing. However, this sampling protocol has rarely been used with EFA despite the clear advantages of doing so.
The second criticism that has been made of the EFA (and all Fourier-based) procedures is that they unnecessary. The point of all Fourier analyses is to estimate the form of a signal — in the case of morphometrics a morphological signal. The Fourier approach provides sophisticated and mathematically elegant tools with which to do this. But that’s all they do. Fourier harmonic amplitudes and phase angles provide a means to describe outline form/shape variation in quantitative terms. But sample ordinations, the major directions of sample form/shape variation, discrimination between sample sub-groups, comparison of patterns of co-variation, form/shape modelling, statistical testing of various sorts, etc. all must be performed on Fourier-based re-descriptions of morphological variation by other procedures. This raises the question of why to take one’s morphological data through a Fourier analysis in the first place as opposed to working directly with the semilandmark outline coordinates themselves as these can easily be aligned and normalized for various sources of extraneous information using other methods (e.g., Bookstein shape coordinates, Procrustes shape coordinates).
As an experiment to address this question empirically we can perform a quick analysis of the same benthic foraminiferal outline data using the Procrustes PCA technique. Results of the projection of the outline shape coordinate data into the spaces formed by the first three eigenvectors of the shape-coordinate covariance matrix the are shown in Figure 7. Close comparison of figures 6 and 7 reveals a few differences (e.g., position of Am. jarvisi along PC-3) which are to be expected considering the differences between the EFA and Procrustes PCA datasets. However, both the gross and detailed similarities between the two ordinations are even more striking. It is doubtful that routine interpretations of these two spaces would differ substantially.
Figure 7. Distribution of the 12 benthic foraminiferan test outlines shown in Figure 4 and Table 2 in the shape space formed by the first three principal components of the covariance matrix calculated between Procrustes superposed shape coordinates. See text for discussion.
Rohlf (1986) argued that Fourier analysis might be preferred to the analysis of coordinates because use of only the first few Fourier harmonics, in effect, causes the outline to be smoother — thus eliminating small scale variation that may not (or may) be of importance in any given analysis. If a sub-set of EFA harmonics are selected for analysis a smoothing of the represented outline would certainly be the case. But Rohlf’s argument strikes me as one that misses the point. If smoothing of an outline is acceptable or important there are many approaches to this operation that could be employed as an initial data-processing step. The most obvious of these is to reduce the number of coordinate points used to represent the boundary form/shape to the minimum needed to achieve an objective geometric tolerance (see MacLeod 1999 for an example algorithm). When this is done it is often surprising how few boundary outline semilandmarks are really necessary to replicate even complex outlines. But once this is done the difference between raw coordinates, Z-R Fourier and EFA become apparent. Taking (say) 50 semilandmarks as an example, the raw analysis of coordinates would imply the analysis of 50 x and 50 y coordinates, 100 variables in total. Under the Z-R Fourier approach 25 amplitudes and 25 phase angles or, more commonly, just the 25 unique harmonic amplitudes would be required, totalling to either 50 or 25 variables respectively. But under EFA each of the 25 unique Nyquist harmonics would require four Fourier coefficients to represent the series, specifying either 100 or 97 variables in total, depending on whether these coefficients were normalized. Of course, the data analyst could simply throw all these EFA variables into a PCA analysis and discard all but the first few principal components as being unimportant. But this standard dimensionality-reduction technique applies equally well to PCA results from raw coordinates, Z-R Fourier shape functions, and indeed to radial Fourier data.
Quite clearly the jury remains out on the question of whether any real advantages are gained by performing a Fourier analysis as a processing step that re-describes the shape in and alternative quantitative format. In this way Z-R Fourier and EFA are reminiscent of principal warps analysis (see MacLeod 2010b). If you are considering using EFA for an outline study I encourage you to explore some of its more unique, yet little-used, variants (e.g., the ability to analyse non-uniformly spaced semilandmarks) in order to add useful and distinctive features to your investigation’s design. But more than this I would recommend you defer the analysis until we have had an opportunity to consider a far more flexible outline sampling - data analysis procedure in detail: eigenshape analysis.
In terms of software, a number of different outline processing, outline digitization, and EFA applications for 2D and 3D data are available from the SUNY Morphometrics web site: http://life.bio.sunysb.edu/morph/. The industry standard in this area, however has to be Jim Rohlf’s EFA application for Windows operating systems. Among the more comprehensive software packages only Jim Rohlf’s NTSYS (http://www.exetersoftware.com/cat/ntsyspc/ntsyspc.html) and Øyvind Hammer’s Past (http://folk.uio.no/ohammer/past/) programme packages have implemented forms of the EFA procedure. All the analyses and graphics used in this column (including the EFA models) were calculated using custom software I have written for Wolfram Researcher’s Mathematica™ software, any or all of which I’d be happy to share on request.
BLACKITH, R. E. and REYMENT, R. A. 1971. Multivariate morphometrics. Academic Press, London 412 pp.
BOOKSTEIN, F. L. 1991. Morphometric tools for landmark data: geometry and biology. Cambridge University Press, Cambridge 435 pp.
BOOKSTEIN, F., CHERNOFF, B., ELDER, R., HUMPHRIES, J., SMITH, G. and STRAUSS, R. 1985. Morphometrics in evolutionary biology. The Academy of Natural Sciences of Philadelphia, Philadelphia 277 pp.
FERSON, S., ROHLF, F. J. and KOEHN, R. K. 1985. Measuring shape variation of two-dimensional outlines. Systematic Zoology, 34, 59–68.
GIARDINA, C. R. and KUHL, R. K. J. 1977. Accuracy of curve approximation by harmonically related vectors with elliptical loci. Computer Graphics and Image Processing, 6, 277–285.
KUHL, R. K. J. and GIARDINA, C. R. 1982. Elliptic Fourier features of a closed contour. Computer Graphics and Image Processing, 18, 236–258.
LESTREL, P. E. 1997. Introduction and overview of Fourier descriptors. In P. E. Lestrel (ed). Fourier Descriptors and Their Applications in Biology. Cambridge University Press, Cambridge, 22–44 pp.
MacLEOD, N. 1999. Generalizing and extending the eigenshape method of shape visualization and analysis. Paleobiology, 25, 107–138.
MacLEOD, N. 2005. Principal components analysis (eigenanalysis & regression 5). Palaeontological Association Newsletter, 59, 42–54.
MacLEOD, N. 2009a. Who is Procrustes and what has he done with my data? Palaeontological Association Newsletter, 70, 21–36.
MacLEOD, N. 2009b. Form & shape models. Palaeontological Association Newsletter, 72, 14–27.
MacLEOD, N. 2010a. Shape models II: the thin plate spline. Palaeontological Association Newsletter, 73, 24–39.
MACLEOD, N. 2010b. Principal & partial warps. Palaeontological Association Newsletter, 74, 35–45.
MacLEOD, N. 2011. Semilandmarks and radial Fourier analysis. Palaeontological Association Newsletter, 76, 25-42.
PIMENTEL, R. A. 1979. Morphometrics: the multivariate analysis of biological data. Kendall/Hunt, Dubuque, IA 275 pp.
ROHLF, F. J. 1986. Relationships among eigenshape analysis, Fourier analysis, and analysis of coordinates. Mathematical Geology, 18, 846–854.
ROHLF, F. J. and ARCHIE, J. W. 1984. A comparison of Fourier methods for the description of wing shape in mosquitoes (Diptera: Culicidae). Systematic Zoology, 33, 302–317.
ROHLF, F. J. and SLICE, D. 1990. Extensions of the Procrustes method for optimal superposition of landmarks. Systematic Zoology, 39, 40–59.
SNEATH, P. H. A. and SOKAL, R. R. 1973. Numerical taxonomy: the principles and practice of numerical classification. W. H. Freeman, San Francisco 573 pp.
ZELDITCH, M. L., SWIDERSKI, D. L., SHEETS, H. D. and FINK, W. L. 2004. Geometric morphometrics for biologists: a primer. Elsevier/Academic Press, Amsterdam 443 pp.
1 This technique was originally named elliptic Fourier analysis (Giardiana and Kuhl 1977), but has also been referred to as elliptical Fourier analysis (e.g., Lestrel 1997).