Multi-scale, structural analysis of geomechanical and petrophysical properties of Permocarboniferous red beds [Elektronische Ressource] = Vielskalige Strukturanalyse der geomechanischen und petrophysikalischen Eigenschaften von Permokarbonischen red beds / von Christian A. Hecht

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Multi-scale, structural analysis of geomechanical and petrophysical properties of Permocarboniferous red beds. Vielskalige Strukturanalyse der geomechanischen und petrophysikalischen Eigenschaften von Permokarbonischen red-beds. Habilitationschrift Zur Erlangung des akademischen Grades vorgelegt der Mathematisch-Naturwissenschaftlich-Technischen Fakultät der Martin-Luther-Universität Halle Wittenberg von von Dr. rer. nat. Christian A. Hecht geb. am: 1.07.1959: in: Herrmannstadt Gutachter/in 1. Prof. Dr. Christof Lempp 2. Prof. Dr. Ulf Bayer, GFZ Potsdam 3. Prof. Dr. Jörn Kruhl, TU MÜnchen Verteidigung: Halle Saale, den 21.11.2003 urn:nbn:de:gbv:3-000006544[http://nbn-resolving.de/urn/resolver.pl?urn=nbn%3Ade%3Agbv%3A3-000006544] 1 Vorwort Die vorliegende Habilitationsschrift ist das Ergebnis meiner, während der letzten sechs Jahre am Institut für Geologische Wissenschaften der Martin-Luther Universität, Halle-Wittenberg durchgeführten Forschungsarbeiten über das Permokarbon. Im Rahmen dieses Forschungsprojektes sind mehrere Diplomkartierungen und eine Diplomarbeit abgeschlossen, sowie eine Dissertation initiiert worden. Die wichtigsten Ergebnisse der bisher geleisteten wissenschaftlichen Arbeit liegen als Publikationen oder Manuskripte vor. Die Form der einzelnen Aufsätze entspricht ihrem status quo zur Zeit der Zusammenstellung dieser Arbeit.

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Publié par	martin-luther-universitat_halle-wittenberg
Publié le	01 janvier 2003
Nombre de lectures	21
Langue	Deutsch

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Vorwort Die vorliegende Habilitationsschrift ist das Ergebnis meiner, während der letzten sechs Jahre am Institut für Geologische Wissenschaften der Martin-Luther Universität, Halle-Wittenberg durchgeführten Forschungsarbeiten über das Permokarbon. Im Rahmen dieses Forschungsprojektes sind mehrere Diplomkartierungen und eine Diplomarbeit abgeschlossen, sowie eine Dissertation initiiert worden. Die wichtigsten Ergebnisse der bisher geleisteten wissenschaftlichen Arbeit liegen als Publikationen oder Manuskripte vor. Die Form der einzelnen Aufsätze entspricht ihrem status quo zur Zeit der Zusammenstellung dieser Arbeit. Der übergeordnete Forschungsansatz des Projektes ist eine skalenübergreifende geomechanisch-geodynamische Betrachtung der besonderen Gesteins- und Gebirgs-eigenschaften des Permokarbons. In einer einfachen Verkettung der vorhandenen Publikationen und Manuskripte würde dieser Forschungsansatzes nicht genügend zum Ausdruck kommen, da die einzelnen Arbeiten thematisch fokussiert sind. Ich habe mich daher entschlossen, die relevanten Publikationen und Manuskripte im Originalformat der jeweiligen Zeitschriften zu verwenden und ausführlich einzuleiten und zu kommentieren. Eine durchgängige Nummerierung der Seiten war dabei nicht möglich, wofür ich um Nachsicht bitten möchte. Ich hoffe mit dieser Darstellungsform einen Weg gefunden zu haben, den Ansprüchen der klassischen Habilitationsschrift und der moderneren kumulativen Habilitation gleichermaßen Rechnung zu tragen. Die hier verwendeten Originalarbeiten sind oder werden in internationalen Fachzeitschriften veröffentlicht und in der Englischen Sprache verfasst. Aus Gründen der sprachlichen Einheitlichkeit und einer möglichen Begutachtung durch nicht Deutsch sprechende Personen wurde für die gesamte Habilitationsschrift die Englischen Sprache bevorzugt. Preface The presented Habilitation thesis is the result of my research work on the Permocarboniferous that I carried out during the last six years at the Department of Geosciences at the Martin-Luther University, Halle-Wittenberg. Within this research project several diploma mapping projects and one diploma thesis were finished and one PHD-thesis was initiated. The essential results of the conducted work are accessible in publications or manuscripts. The papers layouts reflect their status quo at the time when this work was compiled. The general scope of this research project is a geomechanical-geodynamical study of the special rock characteristics of the Permocarboniferous across different scales. The scope of this project would not clearly come out by a simple line up of the papers and manuscripts, because the particular papers concentrate on certain themes. Therefore, I have decided to use the relevant papers and manuscript in the original format of the individual journals but to introduce and commend them in detail. It was not possible to number the pages continuously, for which I want to apologize. I hope that this type of presentation satisfies the requirements of the classical Habilitation thesis as well as the more modern cumulative Habilitation thesis. The original papers are published or to be published in international journals and hence written in English. For reasons of lingual uniformity and of a possible review through not German speaking persons the English language was preferred for the entire Habilitation thesis.

CONTENTS...3 ABSTRACT...5 1. INTRODUCTION.....6 2. CHAPTER 1...13 GEOMECHANICAL MODELS AND PETROPHYSICAL PROPERTIES OF COARSE GRAINED ROCKS. 2.1 Introduction to Chapter 1...14 Paper 1 Hecht, C.A. 2000. Appolonian Packing and Fractal Shape of Grains Improving Geome-chanical Properties in Engineering Geology. Pure appl. geophys. 157, 487-504 Paper 2 Hecht, C. A. 2004. Gomechanical Models for Clastic Grain Packing. Pure appl. geophys. 161, 331-349. Paper 3 Hecht, C. A. and Bönsch, C., Bauch, E. (resubmitted after review) Relations of Rock Structure and Composition to Petrophysical and Geomechanical Rock Properties: Examples from Permocarboniferous red- beds. Rock Mechanics and Rock Engineering. 3. CHAPTER 2.......17 FRACTURE SYSTEMS AND GEOMECHANICAL BEHAVIOUR OF PERMO-CARBONIFEROUS ROCK MASSES. 3.1 Introduction to Chapter 2.......18 Paper 1 Hecht, C. A. 2001. Geomechanical and Petrophysical Properties of Fracture Systems in Permocarboniferous red-beds . Proceedings of the 38Th U.S. Rock Mechanics Symposium, DC Rocks, Washington, 1237-1245. Balkema Rotterdam. Paper 2 Hecht, C. A. 2003. Relations of self-similarity phenomena of multi-scale fracture systems to geomechanical and hydraulic properties of Permocarboniferous red beds. In: Benassi, A., Cohen, S., Istas, J. and Roux, D. (eds) Self Similarity and Applications. Annales de l` Universite de Clermont Ferrand.

4. CHAPTER 3......20 GEOMECHANICAL MODEL FOR THE EVOLUTION OF PERMIAN-MESOZOIC BASINS 4.1 Introduction to Chapter 3...21 Paper 1 Hecht, C. A., Lempp, C. and Scheck, M. (2003) Geomechanical Model for the Post-Variscan Evolution of the Permocarboniferous-Mesozoic Basins in Northeast Germany. Tectonophysics, 373, 125-139. 5. DISCUSSION......22 6. CONCLUSIONS.25 Acknowledgements.....25

ABSTRACT This work comprises analyses of the petrophysical rock properties and the geomechanical behaviour of coarse grained sedimentary rocks on different scales. It covers the scales of rock samples, of rock sequences and of sedimentary basins. The papers and manuscripts are mainly concerned with red-beds of Permocarboniferous age. In essence, the studies relate observations of rock structures and rock compositions to the geomechanical behaviour of rocks and derive principle geomechanical models of complex geological systems. The applied methods include rock description techniques on and across different scales and a wide variety of laboratory testing methods. The results show that similar principles of order and disorder apply on different scales of observation. This study presents a new, scale invariant principle called geomechanical order, which is defined as a function of the structural order and the compositional order of a geological system. Within this work, the principle was applied to systems governed by brittle deformation. The different papers comprise details of the determination of the geomechanical order on different scales and of its relevance for petrophysical properties and for the geomechanical behaviour of rocks. Because rock formation is not a static process the papers also include some considerations on dynamic systems. Because of the limited scale of observation techniques and laboratory testing, the results are limited to the particular scales of the data sets. However, the single contributions also reveal information of geomechanical relations across scale boundaries, for example the relation of sample stiffness to fracture systems. In the context of up-scaling procedures, methods of fractal geometry were applied and their limits and potentials are discussed in some detail. The combination of different approaches with the related methods gives a comprehensive picture of the geomechanical properties of Permocarboniferous red beds. This work contains a number of general theoretical considerations and models, which in particular may also be applicable to other projects of material sciences, engineering geology and structural geology. key words: Permocarboniferous, red beds, rock mechanics, geomechanical behaviour, fracture systems, grain fabrics, scale relations, fractal geometries.

1. INTRODUCTION The general scope of this study is to analyse the relations of structural and geometrical characteristics to the mechanical behaviour of Permocarboniferous rocks and rock units on different scales. The concept of this study follows the geomechanical-geodynamical principle that the petrophysical condition and the geomechanical behaviour of a rock unit is the summary of its compositional features and its strain history. Consequently, the study is concerned with various processes of rock formation, deformation and alteration through time and across scale boundaries. The classical scale of observation in geosciences has been the outcrop scale. As analytical techniques advanced, more and more observations on the lower and higher scales of resolution became possible. Presently the scales of observation in geology reach from the smallest scale of samples for high-resolution methods, across the scale of outcrops to the scale of orogens and basins. Each scale range has its own analytical inventory performed by geoscientists and neighbouring scientific disciplines (Table 1). Scale of observation Methods Scientific disciplines Sample scale Microscopy Geoscience Phase analysis Material science Petrophysical experiments Outcrop scale Sedimentological analysis Geoscience Structural analysis Large-scale experiments Crustal Scale Drilling Geoscience Seismic experiments Geophysics Remote sensing Table 1. Summary of geoscientific methods and disciplines in relation to scales of observation As is largely believed the degree of resolution decreases with increasing scales of observation. In fact, this depends on the point where one starts to look at a system and how far one goes towards lower and higher scales. What is true is that resolution is increasing at any scale as a result of technical progress and that the images that we obtain from modern observation tools contain more and more details. From a fractalists point of view the perfect image of an object

would be infinite towards both ends of the scale so that he or she can zoom through scales and compare structures and objects for phenomena like self-similarity, self affinity or scale invariance. Opposed to human imaginations and computer animations real images are always restricted within certain limits of resolution. Some of them are looking very similar and we are not able to tell the size of the objects on a picture without scale information. This leads us to the presumption that the processes that create similar structures may also be similar. Rocks are static systems and hence the primary observations are static as well. It is not surprising that geological sciences started with the description of rocks and the identification and correlation of similar rock suites across regions and oceans. The classical approach to geology was litho-stratigraphy and bio-stratigraphy. Considering static questions there is less a problem with the reliability of results even if their spatial distribution covers different scales, because the actual observations are not so sensitive to scale transitions. For example, a stratigraphic boundary appears clear in a single borehole, in a perfect 3-D outcrop, as well as in an interpolation between a series of 1 D boreholes that cover a large area. Even though there is a difference in the observation scale and spatial resolution, the quality and reliability of the individual observations are quite similar. Presently geoscientists are rather interested in dynamic processes of rock formation at all available scales. Some dynamic processes can be derived from active geo-environments, from small-scale experiments and from analogous and numerical models. As is well known, the transfer of laboratory results to larger scales causes severe calculation problems. Natural environments and analogous models are scale dependant and hence transformations of results into other scales are problematic. Numerical models are dimensionless on the first view, but the calculation parameters of a certain object that is simulated are scale related empirical results so that the problem of scale dependence remains. Dynamic analyses cause much more problems because the effective system parameters vary through time and space and systems may behave deterministic, random or chaotic. Another big problem is the lack of long-term experiments and large-scale experiments. In fact, we know a little about dynamic processes from comparably fast experiments on the laboratory scale and from a few large-scale experiments but almost nothing about long-term processes on large scales. Natural systems are often irregular and non-isotropic and we can see or measure this even on one scale of observation. Because any observation is more or less scale dependent, the degree of order of an object or system is very difficult to characterize and to quantify across several scales. This is particularly true, if we analyse a rock sequence on many scales, and need to change observation strategies and rock-testing methods at existing scale boundaries. If a system contains distinct scale boundaries across which the petrophysical or structural elements that define the degree of order are not compatible, the attempts of upscaling or

Crustal extension

Thermal subsidence Tectonic subsidence

Diagnostic Data

Seismic profiles Major structures

Rock composition Sedimentation rates

downscaling of results get arbitrary. On the opposite, we observe scale invariance and hierarchical phenomena in geological systems. Scale invariance commonly relates to fractal patterns or systems, which are recognizable by linear correlations of their geometries and parameters on double logarithmic plots. If scale invariance across several orders of magnitude is recognized, the renormalization group method (RNG) can be applied, which means to transform the system equations from one scale to another by changing of their variables. In other words, the same principal model applies on different scales. Summaries of definitions and applications are published in Korvin (1992) and Turcotte 1997). The story becomes interesting at the point when the different steps of data collection and interpretation are connected and we start to analyse the dynamics of the multi-scale system itself. Considering the dynamic evolution of a sedimentary basin a variety of physical processes are involved (Table 2). Stage of basin formation Physical Processes Early basin stage Basin fill Diagenesis Deformation Exhumation Erosion Table 2.processes and data related to basin formation.Summary of From the processes listed in Table 2, it becomes obvious that during the development of a sedimentary basin rather dynamic processes alternate with rather static ones. The intensities of the processes may vary but in essence, these are the steps of a dynamic basin evolution. The different processes also cover different scale ranges and leave diagnostic traces at

Mineral growth

Fault kinematics

Thermal uplift Tectonic uplift

Disaggregation of minerals Fragmentation of rocks

Type of cements Fluid inclusions

Geometry and kinematics of thrusts, faults, folds,

Fault reactivation Joint patterns

Mineral composition Fracture patterns

different scales. The dimension of a diagnostic observation to the assumed process can span several orders of magnitude, for example when fluid inclusion measurements are used for the interpretation of regional diagenetic processes. Other observations, for example strength measurements of a certain rock sample are only valid for the deformation process within the size of the sample. Another interesting scale effect is that time conserved in a geological system increases with increasing scale of observation in a certain direction. In horizontally bedded sedimentary rocks, for example, time increases with the prolongation of the vertical observation axes by adding older strata and processes of millions of years to the system but not on the horizontal observation axes, which represents the uppermost and youngest stratigraphic layers and the processes therein. From a stratigraphy point of view, this is not a very exiting statement but from the point of view of structural analysis of basin dynamics it certainly is, because the vertical axes does contain much more information of the basin evolution than the horizontal axes does. The larger the scale of a geological system in a 3D analysis is, the more important this scale effect gets. The following study characterizes the mechanical behaviour of Permocarboniferous red beds in terms of principal structural characteristics and petrophysical properties from which principal geomechanical laws are derived. One general observation for the rock units investigated in this study is that at any scale the dominant behaviour is brittle which means that the type of deformation is scale-invariant. A principle attempt of this study is to define the characteristic degree of order of the system in two ways. The first, which is called here structural order, is determined at a certain scale by distribution statistics of the systems elements and by the determination of the masses, shapes and sizes of the single elements. Beyond the pure structures and geometries, the degree of order of a system further depends on differences of the petrophysical properties of its elements. This second type of order is the compositional order of the system. Finally, the total degree of order, the geomechanical order of a structure is a function of the geomechanically relevant geometries (structural order) and material properties (compositional order). To give a simple illustrative example we consider two sandstones that have identical grain size distribution curves in other words that have the same structural degree of order. We assume that sandstone number one comprises 95 % of quartz grains and 5% of feldspars and sandstone number two 70 % of quartz grains and 30 % of feldspars. Because quartz grains and feldspars have differing single grain properties for example shape and strength, sandstone number two has a lower degree of geomechanical order because it comprises a higher percentage of weaker elements than sandstone number one. This principle applies to many structures at different scales. The following table contains a summary of examples that are relevant to this study (Table 3).

Sample scale Outcrop scale Crustal scale

Grain size distribution Fracture patterns Fault patterns Packing density Basin geometriesMulti-layer geometries Grain contacts Coordination numbers

Grain composition Fracture properties Fault properties Grain properties Multi-layer properties Basin fill properties

Fabric behaviour Fracture propagation Fault kinematics Fracture connectivity Basin development

Type of order Structural order Compositional order Geomechanical Order Table 3.Theoretical types of order listed for different geological scales of observation. Facing the problem of upscaling one may ask the question: Does the composition of a rock influence or determine the geomechanical behaviour of a single bed, does the single bed behaviour influence the behaviour of a multi-layered rock sequence, does the behaviour of a rock sequence influence the development of a large geological system and so forth? The first attempt to answer this question would be to look at a system with a high degree of order for example a sequence of sandstone layers of similar composition that was subjected to one phase of deformation for example extension. The expected result would be that in a given stress field the statistic spacing distribution and dimensions of the extensional joint set are related to the stiffness of the sandstones and the picture would not be very complicated. Continuing on this example the degree of order can theoretically decrease in two ways. The first way is to add single beds with strongly differing lithologies to the rock sequence, which results in single bed behaviour within the multi-layers through interlayer stress transfer that creates more complex statistic spacing distributions and dimensions of the fracture sets. The second way is to increase the number and styles of applied stress fields, which reactivates existing fractures or produces new ones. The first example represents an increase of the internal structural complexity while the second example gives an increase of the external forces that affect the system. The question in many natural examples is what drives or dominates the self-organisation during the development of a system, the internal or the external parameters. In non-linear geodynamic systems, both parameters discussed above are alternating and balancing each other over time. Local effects such as special lithological features or stress concentration are also important to consider. Going back to the initial question one can answer yes, rock composition does determine the geomechanical behaviour

at any scale because whatever the external forces are the self-organisation ever depends on the internal parameters, even on those at the smallest scales. The key to the understanding of a particular rock system the status quo of which we see and measure presently is to decipher the relations of the relevant driving forces. Firstly, data collections of the details of the internal and external parameters relevant to the scale of the particular system are necessary. Secondly, the data sets must be checked for relations of symmetry, order and disorder and other phenomena such as self-similarity, scale invariance across as many scales as possible. Thirdly, the potential geomechanical behaviour types like deterministic, stochastic or chaotic need to be evaluated. Finally, one may be able to elaborate the linearity of the dynamic evolution of the system for a given time period. Following multi-scale geomechanical/geodynamical aspects this study covers observation scales that reach from the scale of clay minerals to the scale of sedimentary basins for example the Northeast German Basin. We are looking at a time span from the first appearance of red-beds in Upper Carboniferous times to their present status quo. The selected Permocarboniferous basins developed in different tectonic positions in Northeast Germany, Southwest Germany and the Southern Alps. The effects of older basement properties and pre-Permian structures on the basin evolution were also taken into account. In terms of rock condition, the study is mainly concerned with hard rocks, but also with primary grain packing properties of sedimentary rocks, which play an important role in a geodynamical context. One of the repeating concepts in this study is that of fractals. Since the publication of the book The Fractal Nature by Mandelbrot (1976) fractal methods have been widely applied to geological structures. The applicability and wealth of fractal methods, however, has largely been neglected perhaps because in the years when fractals were en vogue many examples of misunderstanding and misapplication were published. Today fractal methods are well confined and their applicability for example in material sciences is unquestioned. Although we know, that many if not most geological structures are not fractal sensu stricto the concepts of fractal geometry have conducted our minds to new principles like hierarchy, self-similarity and scale invariance of geological structures and processes. Fractal principles also deeply support our thoughts about the self-organizing phenomena of dynamic geological processes. One of the perhaps most famous examples of fractal behaviour in geology is fragmentation (for summary see Turcotte 1999). During Permocarboniferous times the mega-continent Pangea, which was finally created by the closure of the Rheic ocean during the Variscan orogeny, started to fall into pieces. This was certainly the beginning of the largest continental fragmentation that has ever taken place on earth. It was associated with extraordinary thermal processes that produced very large