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. 2018 Mar 15;145(6):dev156778. doi: 10.1242/dev.156778

Fig. 2.

Fig. 2.

LOCO-EFA retrieves correctly the cell shape's dominant spatial frequency. (A) EFA decomposes a two-dimensional cell outline into an infinite summation of related ellipses or modes that can also be used to approximate the cell outline. (B) Each EFA harmonic is decomposed into two counter-rotating circles. (C) Mode Inline graphic is composed of the counter-clockwise rotating n+1th harmonic circle and the clockwise rotating n−1th circle. (D) The combined amplitude contribution to Ln (yellow line) of the two counter-rotating circles with radii Inline graphic and Inline graphic also depends on the offset in their starting points and the offset of the overall (mode 1) starting point, which together determine the initial phase shift (green dots) in the amplitude contribution of each rotor. (E,F) Comparison of closed contour reconstruction through either EFA (E) or LOCO-EFA (F). Although both approximations converge to the original six-lobed star shape (labelled ‘Original’), the reconstruction using EFA harmonics (E) generates a spurious shape after addition of the fifth harmonic and only recovers the original shape after the seventh harmonic, whereas the LOCO-EFA (F) reconstitutes the original shape precisely at the sixth mode, matching the protrusion number. The number of modes used for each sequential reconstruction is indicated below each shape. (G) LOCO-EFA reconstruction of a real cell taking the first n Inline graphic modes into account, as indicated below the panels. (H) Determination of the level of mismatch between the original cell shape and the Nth mode truncated LOCO-EFA approximation, by applying the XOR (exclusive OR) function (see supplementary Materials and Methods).