Tímea Szabó’s research while affiliated with Budapest University of Technology and Economics and other places

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Publications (14)


Figure 1 of 11
Examples for equilibrium classes. a1) Gradient field of tri-axial ellipsoid in primary class {2,2}\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\{2,2\}$$\end{document}. a2) Morse-Smale complex associated with the tri-axial ellipsoid. a3) planar drawing of the graph representing the tertiary class of the tri-axial ellipsoid. a4) quasi-dual representation of the complex. b1) Gradient field of a smoothened tetrahedron T in primary class {4,4}\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\{4,4\}$$\end{document}. b2) Morse-Smale complex associated with T. b3) planar drawing of the graph representing the tertiary class of T. b4) quasi-dual representation of the complex
The Morse-Smale complex of a real pebble: primal Morse-Smale graph in class Q3⋆\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\mathcal {Q}}}^{3\star }$$\end{document} a) drawn on the pebble’s surface b) drawn on the plane
Different representations of a Morse-Smale complex. a) Primal Morse-Smale graph in class Q3⋆\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\mathcal {Q}}}^{3\star }$$\end{document} b) Primal Morse-Smale graph with the maxima and minima connected c) Quasi-dual Morse-Smale graph in class Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${{\mathcal {Q}}}$$\end{document}
a) Two splittings of a vertex in quasi-dual representation b) The same vertex splittings in primal representation

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A topological classification of convex bodies
  • Article
  • Full-text available

June 2016

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305 Reads

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18 Citations

Geometriae Dedicata

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Tímea Szabó

The shape of homogeneous, generic, smooth convex bodies as described by the Euclidean distance with nondegenerate critical points, measured from the center of mass represents a rather restricted class M_C of Morse-Smale functions on S^2. Here we show that even M_C exhibits the complexity known for general Morse-Smale functions on S^2 by exhausting all combinatorial possibilities: every 2-colored quadrangulation of the sphere is isomorphic to a suitably represented Morse-Smale complex associated with a function in M_C (and vice versa). We prove our claim by an inductive algorithm, starting from the path graph P_2 and generating convex bodies corresponding to quadrangulations with increasing number of vertices by performing each combinatorially possible vertex splitting by a convexity-preserving local manipulation of the surface. Since convex bodies carrying Morse-Smale complexes isomorphic to P_2 exist, this algorithm not only proves our claim but also generalizes the known classification scheme in [36]. Our expansion algorithm is essentially the dual procedure to the algorithm presented by Edelsbrunner et al. in [21], producing a hierarchy of increasingly coarse Morse-Smale complexes. We point out applications to pebble shapes.

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Figure 1: Mars field setting and the traverse of Curiosity. (a) Gale Crater, with location of the Curiosity landing ellipse. White circle highlights eroded channel feeding the northern crater rim, which has been proposed to be the sediment source for Bradbury Rise conglomerates. Arrow indicates sediment transport direction, red box shows area in b. (b) The landing site (within the red box) and Curiosity's traverse for Sols (Martian days) 0–403 (yellow line) and Sols 403–817 (black dashed line). The Peace Vallis alluvial fan extends down dip and into Curiosity's landing ellipse. The landing ellipse also contains exhumed alluvial fan deposits that predate Peace Vallis, and define a bajada, which once depositionally infilled the crater margin5, 6, 7. Red box shows area in c. (c) Expanded view of Curiosity's traverse for Sols 0–403, with the locations of images studied in this paper (red dots). (d) Rounded pebbles at Sol 27, Link outcrop. Image number: CX00027MR0030530F399886415VA. (e) Rounded pebbles at Sol 356. Image number: 0356MR1452001000E1_DXXX. (f) Angular clasts at Sol 389. Image number: 0389ML1600090000E1_DXXX. On d–f, analysed grains are enhanced with purple colour. Image credits: (a) NASA/JPL-Caltech/ESA/DLR/FU Berlin/MSSS; (b,c) NASA/JPL-Caltech/Univ. of Arizona; (d–f) NASA/JPL-Caltech/MSSS.
Figure 2: Qualitative shape trends from theory and observation. (a) Shape evolution of a single particle constantly colliding with a flat surface is described by Firey’s equation8 ν=cκ, where ν is the speed of abrasion in the inward normal direction, c is a constant and κ is the local curvature. This is illustrated on a quadrangle. b–d show example pebbles from each system studied, with comparable shape parameters as indicated beneath each image (IR: circularity, C: convexity, b/a: axis ratio, ). (b) Sketch of the rotating drum experiment, limestone pebble samples (a≈15–35 mm) and mean shape parameter values after 0, 10.6 and 20.7% mass loss. (c) Aerial image of Dog Canyon fan, example limestone pebble contours (a≈20–40 mm) and mean shape parameter values at x=0, x=1.18 and x=2.10 km. Grains were collected from the active channel denoted by the blue line. (d) A few Martian grain contours (b≈2–32 mm; ref. 2) and mean shape parameter values at Sols 389, 27 and 356. Image credits: (c) Google Earth; (d) NASA/JPL-Caltech/MSSS.
Figure 3: Quantitative shape evolution as a function of mass loss. Upper left insets: definition of shape parameters. (a) Circularity (or isoperimetric ratio), defined as IR=4πA/P2, where A is the area and P is the perimeter of the pebble’s projection in the a−b plane42. (b) Convexity, C=A/Ahull, where Ahull is the area of the convex hull15. (c) Axis ratio, the ratio of the short (b) and long (a) axis lengths. Lower right insets: evolution of shape parameters against transport distance from the apex of Dog Canyon alluvial fan. Neighbouring sites were paired and averaged to form 11 data points from the 22 sites sampled (Methods). Main diagrams show evolution of shape parameters against mass loss in the experiment (black dots), and in the river from Puerto Rico (grey triangles)15. Coloured markers represent mean shape parameter values, with error bars showing the s.e. Rounded Mars pebble values (red markers, Supplementary Table 1) were projected onto the experimental curves (red horizontal arrows) to estimate mass loss (red vertical arrows); the difference in shape values between the two populations is interpreted as inter-site variability rather than a reflection of any trend. Blue markers represent angular clasts from Mars. Dog Canyon results (green and magenta markers) were also projected onto the experimental curves; data suggest particles at fan apex (x=0 km) are slightly abraded due to transport in the upstream canyon (≈5% mass loss), and experience ≈15% mass loss due to bed-load transport over a 2-km distance down the alluvial fan.
Reconstructing the Transport History of Pebbles on Mars

October 2015

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398 Reads

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91 Citations

The discovery of remarkably rounded pebbles by the rover Curiosity, within an exhumed alluvial fan complex in Gale Crater, presents some of the most compelling evidence yet for sustained fluvial activity on Mars. While rounding is known to result from abrasion by inter-particle collisions, geologic interpretations of sediment shape have been qualitative. Here we show how quantitative information on the transport distance of river pebbles can be extracted from their shape alone, using a combination of theory, laboratory experiments and terrestrial field data. We determine that the Martian basalt pebbles have been carried tens of kilometres from their source, by bed-load transport on an alluvial fan. In contrast, angular clasts strewn about the surface of the Curiosity traverse are indicative of later emplacement by rock fragmentation processes. The proposed method for decoding transport history from particle shape provides a new tool for terrestrial and planetary sedimentology.


Universality of fragment shapes

March 2015

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862 Reads

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80 Citations

The shape of fragments generated by the breakup of solids is central to a wide variety of problems ranging from the geomorphic evolution of boulders to the accumulation of space debris orbiting Earth. Although the statistics of the mass of fragments has been found to show a universal scaling behavior, the comprehensive characterization of fragment shapes still remained a fundamental challenge. We performed a thorough experimental study of the problem fragmenting various types of materials by slowly proceeding weathering and by rapid breakup due to explosion and hammering. We demonstrate that the shape of fragments obeys an astonishing universality having the same generic evolution with the fragment size irrespective of materials details and loading conditions. There exists a cutoff size below which fragments have an isotropic shape, however, as the size increases an exponential convergence is obtained to a unique elongated form. We show that a discrete stochastic model of fragmentation reproduces both the size and shape of fragments tuning only a single parameter which strengthens the general validity of the scaling laws. The dependence of the probability of the crack plan orientation on the linear extension of fragments proved to be essential for the shape selection mechanism.



Table 1 . Expected Evolution of Various 3-D and 2-D Shape Descriptors Under Curvature-Dependent Abrasion 
Figure 5. Conceptual illustration of the effects of frictional and collisional abrasion in equations (4) and (5) on the plane S/L-I/L. Sliding drives particles toward infinitely flat shapes (S/L = 0), rolling results in an infinitely thin needle-like shape (S/L = I/L = 0), while collisions between like size particles produce spheres (S/L = I/L = 1). Figure adapted from Domokos and Gibbons [2012].
Figure 6. Map of field site, located within the Luquillo Critical Zone Observatory in northeastern Puerto Rico. The red line outlines the Rio Mameyes watershed, and the blue line denotes the channel. Circles mark sampling sites. Yellow circles represent detailed sampling sites where equilibrium points and axis dimensions were measured in addition to images of pebbles (grain populations A and B). Red circles represent sampling sites where only images of pebbles were taken (grain population C).
Quantifying the Significance of Abrasion and Selective Transport for Downstream Fluvial Grain Size Evolution

November 2014

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477 Reads

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80 Citations

It is well known that pebble diameter systematically decreases downstream in rivers. The contribution of abrasion is uncertain, in part because: (1) diameter is insufficient to characterize pebble mass loss due to abrasion; and (2) abrasion rates measured in laboratory experiments cannot be easily extrapolated to the field. A recent geometric theory describes abrasion as a curvature-dependent process that produces a two-phase evolution: in Phase I, initially blocky pebbles round to smooth, convex shapes with little reduction in axis dimensions; then, in Phase II, smooth, convex pebbles slowly reduce their axis dimensions. Here we provide strong evidence that two-phase abrasion occurs in a natural setting, by examining downstream evolution of shape and size of thousands of pebbles over ~10 km in a tropical montane stream. The geometric theory is verified in this river system using a variety of manual and image-based shape parameters, providing a generalizable method for quantifying the significance of abrasion. Phase I occurs over ~1 kilometer, in upstream bedrock reaches where abrasion is dominant and sediment storage is limited. In downstream alluvial reaches, where Phase II occurs, we observe the expected exponential decline in pebble diameter. Using a discretized abrasion model (the so called “box equations”) with deposition, we deduce that abrasion removes more than 1/3 of the mass of a pebble, but that size-selective sorting dominates downstream changes in pebble diameter. Overall, abrasion is the dominant process in the downstream diminution of pebble mass (but not diameter) in the studied river, with important implications for pebble mobility and the production of fine sediments.



Fluvial Clast

May 2014

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21 Reads

DefinitionA pebble to boulder-size stone transported by flowing water, usually by a river or a stream.SynonymsBed load; Fluvial gravelMorphometryGrain size is most commonly classified according to the Wentworth scale (Wentworth 1922) as follows: >256 mm, boulder; 64–256 mm, cobble; and 2–64 mm, pebble. Particles below 2 mm belong to sand, silt, or clay.Shape is another important morphological aspect of fluvial clasts. A large variety of so-called shape indices have been proposed to describe the overall three-dimensional shape of particles (Blott and Pye 2008*); all these indices are derived from the measurements of the three linear dimensions: the length (a), breadth (b), and thickness (c) of the particles. The most widespread shape indices are the axis ratios b/a and c/b, proposed by Zingg (1935). Beyond length measurements, recent studies show that the number of static equilibria is a natural and clear indicator of the overall clast shape (Domokos et al. 2010). Another frequently use ...


Abrasion model of downstream changes in grain shape and size along the Williams River, Australia

December 2013

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215 Reads

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28 Citations

Modeling pebble abrasion during bed load transport is of fundamental importance in fluvial geomorphology, as it may help to understand downstream fining patterns along gravel bed rivers. Here we review a recently published analytical abrasion model called box equations, which can simultaneously track the shape and size evolution of large pebble populations as the cumulative effect of binary collisions between particles. The model predicts that pebble shapes move away from the sphere and develop sharp edges due to collisional abrasion by sand. We present a field study on the downstream evolution of basalt particle shape and size along the Williams River in the Hunter Valley, Australia. Pebbles get flatter and thinner, and several aquafacts (i.e., abraded pebbles with sharp edges) emerge in the downstream reaches, both suggesting the importance of abrasion by sand. Applying box equations with a few fitted parameters, we present a numerical simulation which reproduces both the shape and size evolution of pebbles along the Williams River. The simulation allows tracking of the shape and size evolution of individual particles as well, revealing an interesting phenomenon that particle size controls shape evolution. Box equations, in combination with existing transport concepts, provide a framework for future shape and size evolution studies in sedimentary environments. In particular, they may help to assess the relative importance of size selective transport versus abrasion in causing downstream fining in gravel bed rivers.


Generating spherical multiquadrangulations by restricted vertex splittings and the reducibility of equilibrium classes

June 2012

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75 Reads

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7 Citations

Periodica Polytechnica Electrical Engineering

A quadrangulation is a graph embedded on the sphere such that each face is bounded by a walk of length 4, parallel edges allowed. All quadrangulations can be generated by a sequence of graph operations called vertex splitting, starting from the path P_2 of length 2. We define the degree D of a splitting S and consider restricted splittings S_{i,j} with i <= D <= j. It is known that S_{2,3} generate all simple quadrangulations. Here we investigate the cases S_{1,2}, S_{1,3}, S_{1,1}, S_{2,2}, S_{3,3}. First we show that the splittings S_{1,2} are exactly the monotone ones in the sense that the resulting graph contains the original as a subgraph. Then we show that they define a set of nontrivial ancestors beyond P_2 and each quadrangulation has a unique ancestor. Our results have a direct geometric interpretation in the context of mechanical equilibria of convex bodies. The topology of the equilibria corresponds to a 2-coloured quadrangulation with independent set sizes s, u. The numbers s, u identify the primary equilibrium class associated with the body by V\'arkonyi and Domokos. We show that both S_{1,1} and S_{2,2} generate all primary classes from a finite set of ancestors which is closely related to their geometric results. If, beyond s and u, the full topology of the quadrangulation is considered, we arrive at the more refined secondary equilibrium classes. As Domokos, L\'angi and Szab\'o showed recently, one can create the geometric counterparts of unrestricted splittings to generate all secondary classes. Our results show that S_{1,2} can only generate a limited range of secondary classes from the same ancestor. The geometric interpretation of the additional ancestors defined by monotone splittings shows that minimal polyhedra play a key role in this process. We also present computational results on the number of secondary classes and multiquadrangulations.


The genealogy of convex solids

April 2012

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67 Reads

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4 Citations

The shape of homogeneous, smooth convex bodies as described by the Euclidean distance from the center of gravity represents a rather restricted class M_C of Morse-Smale functions on S^2. Here we show that even M_C exhibits the complexity known for general Morse-Smale functions on S^2 by exhausting all combinatorial possibilities: every 2-colored quadrangulation of the sphere is isomorphic to a suitably represented Morse-Smale complex associated with a function in M_C (and vice versa). We prove our claim by an inductive algorithm, starting from the path graph P_2 and generating convex bodies corresponding to quadrangulations with increasing number of vertices by performing each combinatorially possible vertex splitting by a convexity- preserving local manipulation of the surface. Since convex bodies carrying Morse-Smale complexes isomorphic to P_2 exist, this algorithm not only proves our claim but also defines a hierarchical order among convex solids and general- izes the known classification scheme in [35], based on the number of equilibria. Our expansion algorithm is essentially the dual procedure to the algorithm presented by Edelsbrunner et al. in [19], producing a hierarchy of increasingly coarse Morse-Smale complexes. We point out applications to pebble shapes.


Citations (12)


... Indeed, since the restriction of ρ K to a plane coincides with the radial function of the intersection of K with the plane, and a similar observation holds for h K and the projection of K onto the plane, it is sufficient to show our remark for plane convex bodies. For this case a simple geometric argument shows the statement (see also [2,31]). We note that the properties that h K or ρ K are C 1 -class are not equivalent [100], but if both are C 1 -class, their critical points coincide. ...

Reference:

Centroids and equilibrium points of convex bodies
A topological classification of convex bodies

Geometriae Dedicata

... Particle shape and gradation (i.e., particle size and particle size distribution) are the fundamental physical parameters of gravelly soils. These parameters not only influence interparticle interactions and the mechanical properties of gravelly soils [8, 10, 11, 19-23, 40, 44, 45, 47, 48, 59, 61, 62, 68, 69] but also reflect the evolutionary history and geological genesis of gravelly soils to some extent [6,14,27,41,54]. Traditionally, the gradation is obtained by sieve test and has many shortcomings and limitations. ...

Reconstructing the Transport History of Pebbles on Mars

... In three dimensions, we have I = (6 √ πV )/(A 3/2 ) where V is the volume and A is the surface area of the solid. The isoperimetric ratio I has been measured both in the field (Miller et al. 2014) and in laboratory experiments (McCubbin et al. 2014). The isoperimetric ratio I is of particular interest, because in case of the v = κ curvature-driven flow (serving as a special model of collisional abrasion) it was proven by Gage (1983) that I(t) is growing monotonically in time. ...

ALTERATION OF SEDIMENTARY CLASTS IN MARTIAN METEORITE NORTHWEST AFRICA 7034
  • Citing Conference Paper
  • September 2014

Meteoritics & Planetary Science

... When these dimensions are relatively similar to each other, the particle tends to be close to spherical, referred to as fragments hereafter. In such particles, equancy, defined as H/L, approaches unity (Szabó and Domokos, 2010). Platelike particles are characterized by high values of platiness, (W -H)/L, a ratio quantifying the difference between the smallest dimension (H) and the other two (L and W). ...

A new classification system for pebble and crystal shapes based on static equilibrium points

Central European Geology

... Geometric models of the high energy (fragmentation) phase and of the low energy (abrasion) phase have been studied in considerable detail. In the case of fragmentation, geometric models consider the bisection of convex polyhedra by random planes and study the combinatorial and metric properties of the descendant polyhedra [2,7,8]. In the case of abrasion, considering the limit where collision energy approaches zero led to the study of mean field geometric partial differential equations (PDEs) [3,5,15,16], describing the evolution of shape as a function of continuous time. ...

Universality of fragment shapes

... Particle shape and gradation (i.e., particle size and particle size distribution) are the fundamental physical parameters of gravelly soils. These parameters not only influence interparticle interactions and the mechanical properties of gravelly soils [8, 10, 11, 19-23, 40, 44, 45, 47, 48, 59, 61, 62, 68, 69] but also reflect the evolutionary history and geological genesis of gravelly soils to some extent [6,14,27,41,54]. Traditionally, the gradation is obtained by sieve test and has many shortcomings and limitations. ...

Quantifying the Significance of Abrasion and Selective Transport for Downstream Fluvial Grain Size Evolution

... Examples of transport mechanisms associated with fragmentation, fatigue failure, and pure chipping are rockfalls, debris flows, and bed-load transport, respectively. Fragmentation figure is adapted from Salman et al. (2004b); chipping figure is adapted from Szabó et al. (2013); photographs of transport mechanisms are reproduced from Wikimedia Commons. each with distinct micro-mechanical failure modes. ...

Abrasion model of downstream changes in grain shape and size along the Williams River, Australia
  • Citing Article
  • December 2013

... The counts we obtained were compared with existing counts of quadrangulations. In the literature we only found counts for n ≤ 12 in the most general case, see Cantarella et al. (2016); Kápolnai et al. (2012), so this check could not be done for higher numbers of vertices. There are however theoretical formulas for the number of quadrangulations with n vertices up to orientation-preserving automorphism, see Liskovets (2000), and the number of rooted quadrangulations, see Sloane (2014). ...

Generating spherical multiquadrangulations by restricted vertex splittings and the reducibility of equilibrium classes

Periodica Polytechnica Electrical Engineering

... Similarly, a convex body K with a significantly flattened or elongated bounding box may not have equilibrium points but in some small regions of bd K including two small patches and a narrow ring as demonstrated by [34]. However, the number of equilibria within these areas can be arbitrary. ...

Pebbles, Shapes, and Equilibria

Mathematical Geosciences

... We call the class of convex bodies with isomorphic abstract graphs the secondary equilibrium class and the class of convex bodies with homeomorphic embedded graphs the tertiary equilibrium class associated with K. See Figure 3(a), which also illustrates that a primary class can contain different secondary classes: e.g., the ellipsoid is not alone in class {2, 2}. In [8] it was shown that the secondary and tertiary schemes are also complete in the sense that no secondary or tertiary class is empty. Metagraph G with vertices at tertiary classes and edges corresponding to codimension 1 bifurcations; thin edges: saddle-nodes, thick edges: saddle-saddle bifurcations. ...

The genealogy of convex solids