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Series: Geological Society, London, Special Publications
Published: 17 July 2024
DOI: 10.1144/SP546-2023-63
EISBN: 9781786206435
... the consequences of violating the little-studied assumption that the focal mechanisms have diverse orientations. Our approach is to employ data-informed synthetic mechanisms, with nodal plane orientations defined by recent earthquake lineaments in the Midland Basin, western Texas, and rakes consistent with slip...
FIGURES | View All (13)
Journal Article
Published: 01 August 1980
Bulletin of the Seismological Society of America (1980) 70 (4): 985–998.
...Jorge A. Mendiguren abstract The composite nodal plane solution method fails when it is applied to a region where the events have different source mechanism in different areas. Presented here is a systematic procedure to delimit those areas and find their particular source mechanism. In its first...
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Strike versus rake plot of the nodal planes derived from focal mechanism analysis of the third-party catalog events for fault system 2. Filled black circles are the results as given by the focal mechanism analysis. Rake values of the gray-filled shapes are calculated for the strike and dip values of the nodal planes as illuminated by stress states with Aφ values of 0.5 to 1. Vertical arrow indicates the azimuth of SHmax for the focal mechanism dataset.
Published: 17 September 2024
Figure 12 Strike versus rake plot of the nodal planes derived from focal mechanism analysis of the third-party catalog events for fault system 2. Filled black circles are the results as given by the focal mechanism analysis. Rake values of the gray-filled shapes are calculated for the strike
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Rose diagrams of the strike of nodal planes for normal faults and normal faults with a strike-slip component (a), strike-slip faults, strike-slip faults with a normal or reverse component (b), reverse faults and reverse faults with a strike-slip component (c).
Published: 01 September 2024
Fig. 5. Rose diagrams of the strike of nodal planes for normal faults and normal faults with a strike-slip component ( a ), strike-slip faults, strike-slip faults with a normal or reverse component ( b ), reverse faults and reverse faults with a strike-slip component ( c ).
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Fitted model of RSS with nodal planes corresponding to strike-slip focal mechanisms. The beach balls shown in Figure 9 are classified according to the stress regime or nodal plane geometry. Compression and tension regions are indicated by red and green regions, respectively. The orientation of the structure is provided in the upper left panel. For reference, the internal friction angle (φ) is obtained from Barton and Choubey (1977) and Yu et al. (2022).
Published: 13 August 2024
Figure 10. Fitted model of RSS with nodal planes corresponding to strike-slip focal mechanisms. The beach balls shown in Figure  9 are classified according to the stress regime or nodal plane geometry. Compression and tension regions are indicated by red and green regions, respectively
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Rose diagram distribution of strike direction and dip angle of nodal planes from FMS of (a) all events, (b) only events with Mw ≥ 5, (c) only extensional events, (d) only strike‐slip (SS) events, and (e) principal stress orientations in the study area obtained by stress tensor inversion of all available FMS.
Published: 30 July 2024
Figure 3. Rose diagram distribution of strike direction and dip angle of nodal planes from FMS of (a) all events, (b) only events with M w ≥ 5, (c) only extensional events, (d) only strike‐slip (SS) events, and (e) principal stress orientations in the study area obtained by stress tensor
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(a) Mohr circle of all ETSZ focal mechanism nodal planes (gray dots) and the most geomechanically favorable plane for each event (black dots). Many of the nodal planes that reproduce first‐motion polarities are nonetheless incompatible with frictional slip. These planes are inadmissible to stress inversions. By contrast, all of the favorable planes are geomechanically viable. (b) Slip potential of ETSZ faults. Polar contour plot of dCFS as a function of fault orientation (dCFS = friction × |normal traction gradient| − |shear traction gradient|), which is the difference between the critical shear stress and the resolved shear stress. The dashed black lines indicate hydrofracture gradient or the limit of slip compatibility. The gray dots indicate the strike and dip of nodal planes from all ETSZ focal mechanisms. Notably, many are slip incompatible. The black circles indicate geomechanically favorable solution for each earthquake. All of these planes are compatible with slip. The color version of this figure is available only in the electronic edition.
Published: 16 March 2023
Figure 3. (a) Mohr circle of all ETSZ focal mechanism nodal planes (gray dots) and the most geomechanically favorable plane for each event (black dots). Many of the nodal planes that reproduce first‐motion polarities are nonetheless incompatible with frictional slip. These planes are inadmissible
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Mohr circles and stereonets of most of the favorably oriented nodal planes from the focal mechanism inversion. The red poles in the Mohr diagrams and the planes in the stereonets correspond to the planes that are expected to slip with the given pore pressure perturbation (shown in each row above the red arrow between the x-intercept of the failure envelope and the original pore pressure value).
Published: 12 July 2021
Figure 6. Mohr circles and stereonets of most of the favorably oriented nodal planes from the focal mechanism inversion. The red poles in the Mohr diagrams and the planes in the stereonets correspond to the planes that are expected to slip with the given pore pressure perturbation (shown in each
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Rose diagrams of (a) strike and (b) dip angles of the nodal planes of the CMT solutions aligned with relocated earthquakes. Nodal planes in groups 2, 4, 7, and 8 are excluded, because earthquakes in these groups are inadequate to constrain fault planes. (c) Stress map of the EF region showing maximum horizontal stress (SHmax) orientations (red bars with arrows) of earthquake groups 1, 3, 5, 6, 9, and 10. Bars only indicate the orientations and exclude magnitude information. The color version of this figure is available only in the electronic edition.
Published: 02 June 2021
Figure 4. Rose diagrams of (a) strike and (b) dip angles of the nodal planes of the CMT solutions aligned with relocated earthquakes. Nodal planes in groups 2, 4, 7, and 8 are excluded, because earthquakes in these groups are inadequate to constrain fault planes. (c) Stress map of the EF region
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Distribution of nodal planes of FM for Chile from the Global Centroid Moment Tensor catalog between 1976 and 2019. FMs are represented in the strike–rake plane (lower right). The shape of the clusters depends on the dip, the shallower the dip, the more elongated the clusters. The model based on Angular Classification with Expectation–maximization (ACE) identifies four clusters: two for interface (in the upper half, with positive rakes) and intraslab (in the lower half, with negative rakes), respectively. The remaining scattered data are unclassified. Those events have mainly hypocenters in the South American crust. The color saturation corresponds to the probability of a nodal plane to be in a certain cluster. For each event, the probabilities of both nodal planes are averaged and used as weights for the event classification used in ground‐motion modeling. The color version of this figure is available only in the electronic edition.
Published: 14 July 2020
Figure 2. Distribution of nodal planes of FM for Chile from the Global Centroid Moment Tensor catalog between 1976 and 2019. FMs are represented in the strike–rake plane (lower right). The shape of the clusters depends on the dip, the shallower the dip, the more elongated the clusters. The model
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Rose diagrams of nodal planes of shear components (left) and map view of event mechanisms with strike angles within 10° of the strike of the maximum horizontal stress. The size of the beach balls is proportional to the event magnitude.
Published: 01 March 2020
Figure 7. Rose diagrams of nodal planes of shear components (left) and map view of event mechanisms with strike angles within 10° of the strike of the maximum horizontal stress. The size of the beach balls is proportional to the event magnitude.
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Lower stereographic projections of (a) nodal planes for the 15 focal mechanisms. Two clusters of nodal planes are identified and found to coincide with the planar structures indicated in Figure 2. (b) Poles to nodal planes, contoured by density. The two clusters are again identified, and the pole to the best-fit plane (225°/25°) determined from the hypocentral distribution is indicated by the green star. (c) P‐ and T-axes of stress inversion colored in blue and red, respectively. (d) Orientation of maximum (σ1, red) and minimum (σ3, blue) compressive stress directions compared against the stress inversion for region B1 of Wada et al. (2010) in black.
Published: 27 August 2019
Figure 4. Lower stereographic projections of (a) nodal planes for the 15 focal mechanisms. Two clusters of nodal planes are identified and found to coincide with the planar structures indicated in Figure  2 . (b) Poles to nodal planes, contoured by density. The two clusters are again identified
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(a) The Coulomb static stress change computed on the nodal planes of the entire catalog of aftershocks analyzed in this study. Positive circles (80%) are events with mechanisms in which one or both nodal planes correspond positively with the Coulomb static stress hypothesis. Negative circles (20%) represent seismicity that is not triggered by the Coulomb static stress change induced by the mainshock (neither nodal plane is favored for failure). (b) Histograms showing the distribution of positive and negative CFS on the nodal plane of the aftershocks as a function of friction coefficient.
Published: 02 May 2017
Figure 8. (a) The Coulomb static stress change computed on the nodal planes of the entire catalog of aftershocks analyzed in this study. Positive circles (80%) are events with mechanisms in which one or both nodal planes correspond positively with the Coulomb static stress hypothesis. Negative
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Stereonet plot of the nodal planes of moment tensor results and the fractures/faults observed from image logs in nearby wells.
Published: 18 July 2016
Figure 6. Stereonet plot of the nodal planes of moment tensor results and the fractures/faults observed from image logs in nearby wells.
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Coulomb stress change resolved on focal mechanism nodal planes. (a) Selection of the most positive Coulomb stress change value from each pair of nodal planes: positive stress change percentage is 87.3% (343 events). (b) Selection of the most positive Coulomb stress change value from each pair of nodal planes: symbols show positive and negative values. Note that μ′=0.8. The color version of this figure is available only in the electronic edition.
Published: 08 September 2015
Figure 16. Coulomb stress change resolved on focal mechanism nodal planes. (a) Selection of the most positive Coulomb stress change value from each pair of nodal planes: positive stress change percentage is 87.3% (343 events). (b) Selection of the most positive Coulomb stress change value from
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(a) Example of the equivalency of nodal planes. The point‐source radiation pattern of the two mechanisms is the same, but the triplets (strike, dip, rake) are different. (b) The two mechanisms are similar, but the parameter triplets are different, as for the vertical faults (dip close to 90°), there is uncertainty in the direction of the fault. The color version of this figure is available only in the electronic edition.
Published: 04 February 2014
Figure 4. (a) Example of the equivalency of nodal planes. The point‐source radiation pattern of the two mechanisms is the same, but the triplets (strike, dip, rake) are different. (b) The two mechanisms are similar, but the parameter triplets are different, as for the vertical faults (dip close
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The first line shows the azimuth and dip of the two nodal planes of every focal mechanism (in black). The reduced dataset orientations are shown in grey. At the bottom, the P and T axes of the 39 focal mechanisms are plotted.
Published: 01 July 2013
Fig. 4 The first line shows the azimuth and dip of the two nodal planes of every focal mechanism (in black). The reduced dataset orientations are shown in grey. At the bottom, the P and T axes of the 39 focal mechanisms are plotted.
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Comparison of the most favorable slip direction from the two nodal planes for the 44 earthquake focal mechanisms in the Pyrenees reported in Table 1 and Figure 6, with the shear stress direction in the fault plane deduced from the second spatial derivative of the geoid.
Published: 01 June 2013
Figure 9. Comparison of the most favorable slip direction from the two nodal planes for the 44 earthquake focal mechanisms in the Pyrenees reported in Table 1 and Figure 6 , with the shear stress direction in the fault plane deduced from the second spatial derivative of the geoid.
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Rose diagram of dip of nodal planes of LRG focal mechanisms determined by ROB. East‐dipping faults plot in the right quadrant, west‐dipping faults in the left quadrant. (a) All nodal planes; (b) preferred nodal planes, based on compatibility with regional stress field. The gray shades correspond to magnitude intervals in the legend; concentric circles correspond to the number of nodal planes per dip angle bin.
Published: 01 April 2013
Figure 7. Rose diagram of dip of nodal planes of LRG focal mechanisms determined by ROB. East‐dipping faults plot in the right quadrant, west‐dipping faults in the left quadrant. (a) All nodal planes; (b) preferred nodal planes, based on compatibility with regional stress field. The gray shades
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Rose diagram of strike of nodal planes of LRG focal mechanisms determined by ROB. (a) All nodal planes; (b) preferred nodal planes, based on compatibility with regional stress field. The azimuth bin width is 20°; gray shades correspond to the magnitude intervals in the legend. The concentric circles indicate the number of nodal planes per azimuth bin.
Published: 01 April 2013
Figure 10. Rose diagram of strike of nodal planes of LRG focal mechanisms determined by ROB. (a) All nodal planes; (b) preferred nodal planes, based on compatibility with regional stress field. The azimuth bin width is 20°; gray shades correspond to the magnitude intervals in the legend