18-Geol-A4 Structural Geology · May 2018
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Reference texts: Davis & Reynolds, Structural Geology of Rocks and Regions (3rd ed.); Fossen, Structural Geology (2nd ed.); Marshak & Mitra, Basic Methods of Structural Geology.
Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.
Given. Twenty True/False statements spanning stress and strain theory, fold and fracture classification, and crystal-defect (dislocation) terminology.
Find. The correct True/False call for each statement, with the one-line reasoning that would earn the mark on a national exam.
| # | Statement | Answer | Reasoning |
|---|---|---|---|
| 1 | Rocks that have undergone purely dip slip faulting can show evidence of strike separation. | True | Separation is measured on an arbitrarily-oriented marker surface (e.g. a dipping bed), not along the true slip vector. A purely dip-slip net slip can still produce an apparent horizontal (strike) offset where it crosses a non-vertical, non-slip-parallel marker — separation and slip are only the same thing for a marker line parallel to net slip. |
| 2 | Axial planar cleavage of a fold forms during the homogeneous strain stage of fold development. | True | Buckling itself is a heterogeneous (layer-parallel-shortening then flexural) process; axial-planar cleavage is imposed by a later, approximately homogeneous flattening strain oriented perpendicular to the axial surface, which is why cleavage fans only slightly and is sub-parallel to the axial surface across the whole fold. |
| 3 | The fold axis connects points of maximum curvature for non-cylindrical folds. | False | That describes the hinge line, which exists for any fold. A true fold axis — a single line direction that can be translated parallel to itself to generate the entire folded surface — is only defined for CYLINDRICAL folds; non-cylindrical folds have no single axis direction. |
| 4 | In theory, buckling involving flexural slip folding produces only Class 1B folds. | True | Flexural slip (and flexural flow) folding preserves orthogonal layer thickness around the fold (parallel folding), which is the defining geometry of Ramsay Class 1B. |
| 5 | Stress traction refers to stress at a point. | False | Traction is the force per unit area resolved on ONE specific plane through a point. The complete state of stress at a point requires the stress tensor (tractions on every possible plane), not a single traction vector. |
| 6 | Mode 1 fractures only form perpendicular to \(\sigma_1\). | False | Mode I (opening) fractures form perpendicular to \(\sigma_3\) (parallel to \(\sigma_1\)-\(\sigma_2\)) — they open against the least compressive stress, not perpendicular to the greatest. |
| 7 | Mode 2 fractures have displacement perpendicular to the fracture front. | True | Mode II is in-plane shear: the two crack faces slide past each other in the fracture plane, in the direction perpendicular to the propagating crack front (Mode III sliding is parallel to the front). |
| 8 | A Mode I fracture may form from either positive or negative normal stresses. | True | A joint/vein opens under net tension, but hydraulic fracturing shows Mode I opening can also occur under a nominally compressive \(\sigma_3\) once elevated pore pressure drives the EFFECTIVE normal stress to the tensile failure condition. |
| 9 | For ideally plastic material strain is linearly related to stress. | False | Ideal plasticity means strain increases at CONSTANT stress once yield is reached — the opposite of a proportional (linear, elastic/Hookean) stress-strain relation. |
| 10 | An intersection lineation between bedding and cleavage provides the orientation of the axial surface. | False | A bedding-cleavage intersection lineation is PARALLEL TO THE FOLD AXIS (a single line), not the axial surface (a plane, needing strike and dip). |
| 11 | Solid state diffusion involving Nabarro-Herring creep occurs along grain boundaries. | False | Nabarro-Herring creep is diffusion THROUGH the grain interior (lattice/volume diffusion); diffusion along grain boundaries is Coble creep. |
| 12 | The same bedding contact can intersect the axial planar cleavage of a fold only once. | False | A bedding surface threading through a periodic fold train (or around both limbs of one fold) crosses the fanning axial-planar cleavage once per hinge zone it passes through, i.e. potentially many times. |
| 13 | An intersection lineation between bedding and cleavage provides the orientation of the axial surface. (repeated in source) | False | Same statement as item 10 above (a duplicate in the printed paper — flagged rather than silently answered differently); the reasoning is identical: an intersection lineation gives the fold-axis line, not the axial-surface plane. |
| 14 | Lines that represent the principal strain axes were perpendicular before the strain. | False (in general) | True only for COAXIAL (pure shear) strain, where material lines that become principal axes never rotate. In non-coaxial strain (e.g. simple shear) the material lines that end up as the finite principal strain axes were NOT mutually perpendicular before straining, because they rotate progressively through the deformation. |
| 15 | Finite strain represents the total accumulated strain for a given period of time. | True | Finite strain is the TOTAL strain from the undeformed to the final state, as distinct from incremental (instantaneous) strain accrued during one small step of the deformation path. |
| 16 | The stress tensor can be fully defined by 6 different components of stress. | True | The 3×3 stress tensor is symmetric (\(\sigma_{ij}=\sigma_{ji}\)), so only 3 normal + 3 shear = 6 independent components are needed. |
| 17 | A screw dislocation is oriented parallel to the Burgers vector. | True | By definition: a screw dislocation's line is parallel to \(\mathbf{b}\); an edge dislocation's line is perpendicular to \(\mathbf{b}\). |
| 18 | The yield point in a rock deformation experiment is the onset of inelastic deformation. | True | The yield point marks the transition from recoverable elastic strain to permanent (plastic or brittle) deformation. |
| 19 | Principal strain axes for simple shear have some component of net angular shear. | True | Simple shear is non-coaxial: the material lines that end up parallel to the finite principal strain axes rotate throughout the deformation path (unlike pure shear, where principal-axis material lines never experience angular shear), so tracked over the whole history they record a net angular shear. |
| 20 | Plane strain is a product of non-coaxial strain. | False | Plane strain is a GEOMETRIC classification of the strain ellipsoid (one principal strain = 0) and is completely independent of the deformation PATH — both pure shear (coaxial) and simple shear (non-coaxial) commonly produce plane strain. |