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Shear Band Length - Displacement Scaling

Generally, shear band lengths and displacements are related, albeit this relationship is some what different than the displacement-length relationship for faults, which apparently form by different mechanisms and generally the published statistical data from faults do not include the faulting mechanism. See 'Scaling between Fault Length and Fault Maximum Slip.' Figure 1 shows some data from several shear bands in the Entrada Sandstone exposed at the San Rafael Desert, Utah (Fossen and Hesthammer, 1997). For bands consisting of a single segment, almost all displacement profiles exhibit upward-convex shape. The displacement maximum may be located in the central portion of the bands.

Plot of length vs displacement measurements for isolated shear bands in Jurassic Entrada sandstone, Uath. From Fossen and Hesthammer (1997).Figure 1. Plot of length vs displacement measurements for isolated shear bands in Jurassic Entrada sandstone, Uath. From Fossen and Hesthammer (1997).

For shear band zones composed of multiple sub-parallel echelon segments (Figure 2), the authors distinguished two types: soft-linked, where segments are not in physical contact, and hard-linked, where segments touch each other (see Walsh and Watterson, 1991 for terminalogy, and Carthright, 1995, for the evolution of the slip distribution along normal faults). The two types differ presumably in the way strain is transferred from one segment to another, either ductilly across soft-linked zones or brittlely across hard-linked zones.

Normalized length plotted against normalized displacement for isolated shear bands (a) and soft-linked shear bands (b). The solid lines in both figures are the best fit third-order polynomial to the data. Apparently the two populations show different trends. From Fossen and Hesthammer (1997).Figure 2. Normalized length plotted against normalized displacement for isolated shear bands (a) and soft-linked shear bands (b). The solid lines in both figures are the best fit third-order polynomial to the data. Apparently the two populations show different trends. From Fossen and Hesthammer (1997).

For soft-linked zones, segments develop individually until a degree of overlap is reached, resulting in a combined system. The displacement profiles (Figure 3) corresponding to this process evolve from a multipeak type, through a plateau type, and will eventually be a coherent single peak type. At the soft-linked stage, the majority of the profiles show steeper gradient towards the tip in the overlap zone than towards the independent tip, similar to what was described for weakness-based faults (see Willemse et al., 1996). The schematic development of a displacement profile along a hard-linked shear band zone is similar to that of a soft-linked zone, from multipeak-type, followed by plateau-type, to single peak profile if growth occurs without further linkage. Figure 3 shows some example profiles of hard-linked zones.

Displacement profiles of soft-linked (a and b) and hard-linked (c and d) systems of shear bands measured in the Jurassic Entrada Sandstone of San Rafael Desert, Utah. From Fossen and Hesthammer (1997).Figure 3. Displacement profiles of soft-linked (a and b) and hard-linked (c and d) systems of shear bands measured in the Jurassic Entrada Sandstone of San Rafael Desert, Utah. From Fossen and Hesthammer (1997).

Figure 4 shows a length-displacement log-log plot for shear bands within the Entrada Sandstone referenced above (Fossen and Hesthammer, 1997). A best fit linear line has a slope of 0.54, which is much smaller than faults reported by others. Figure 5 shows a log-log plot of displacement-length data from shear bands in carbonate grainstone exposed in the island of Favignana, west of Sicily (From Tondi et al., JSG in review). The data shows linear trends for single shear bands, zones of shear bands, and shear band zones with slip surfaces. However, there are strikingly noticeable jumps from one data set to another implying well-defined forms in the scaling properties as the structures evolve from simple shear bands, to shear band zones, and finally to shear band zones with slip surfaces.

Log-log plot of the displacement-length data from the San Rafael Desert, Utah, showing a linear trend with a best fit line with a slope of 0.54. From Fossen and Hesthammer (1997).Figure 4. Log-log plot of the displacement-length data from the San Rafael Desert, Utah, showing a linear trend with a best fit line with a slope of 0.54. From Fossen and Hesthammer (1997).
Log-log plot of the displacement-length data from compactive shear bands in carbonate grainstone cropping out in the island of Favignana, west of Sicily, for single bands (blue), zones of bands (red), and bands with slip surfaces (green). They have linear trends where the best fit lines are shown but there are jumps between data sets indicating the evolution of the shear band fault system. From Tondi et al. (2012).Figure 5. Log-log plot of the displacement-length data from compactive shear bands in carbonate grainstone cropping out in the island of Favignana, west of Sicily, for single bands (blue), zones of bands (red), and bands with slip surfaces (green). They have linear trends where the best fit lines are shown but there are jumps between data sets indicating the evolution of the shear band fault system. From Tondi et al. (2012).
Reference:

Cartwright, J.A., Trudgill, B.D., Mansfield, C.S., 1995. Fault growth by segment linkage; an explanation for scatter in maximum displacement and trace length data from the Canyonlands Grabens of SE Utah. Journal of Structural Geology 17: 1319–1326.

Fossen, H., Hesthammer, J., 1997. Geometric analysis and scaling relations of deformation bands in porous sandstone. Journal of Structural Geology 19(12): 1479-1493.

Tondi, E., Cilona, A., Agosta, F., Aydin, A., Rustichelli, A., Renda, P., Giunta, G., 2012. Growth processes, dimensional parameters and scaling relationships of two conjugate sets of compactive shear bands in porous carbonate grainstones, Favignana Island, Italy. Journal of Structural Geology 37: 53-64.

Walsh, J.J., Watterson, J., 1991. Geometric and kinematic coherence and scale effects in normal fault systems. In the Geometry of Normal Faults, eds A.M. Roberts, G. Yielding and B. Freeman. Geological Society of London Special Publication 56: 193-203.

Willemse, E.J.M, Pollard, D.D., Aydin, A., 1996. Analysis of the relationship between slip distribution and 3D echelon fault geometry with consequences for fault scaling. Journal of Structural Geology 18 (2-3): 295-309.



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