The Calculation of Safety Front Boundary of Paired Approach Procedure Based-on Escape Maneuver

Author(s):  
X. He ◽  
F. Zhang ◽  
J. Chen ◽  
F. Song
Keyword(s):  
1987 ◽  
Vol 24 (8) ◽  
pp. 1507-1525 ◽  
Author(s):  
W. M. Schwerdtner

Grenville gneiss of the central Georgian Bay region was subjected to ductile deformation that produced narrow mylonite zones as well as three sets of superimposed folds differing greatly in structural signature, size, and orientation. Some mylonite zones are concordant to gneissosity and are repeatedly folded, others cut gneissosity and postdate the folding. Gneissosity was generated as a regionally subhorizontal feature, either by crustal thinning or, like the early mylonite zones, by low-angle reverse shearing. An attempt is made to account for the initially subhorizontal gneissosity, the mylonite zones, and the folds in a regime of large-scale reverse shearing that strikes parallel to the Grenville Front.Upright northwest–southwest to north–south buckle folds dominate the map pattern and are subperpendicular to the reverse Grenville Front boundary fault. These set-2 folds cannot be attributed to reverse simple shearing but require a large component of east–west compression. Such stress could have been generated in a northwest–southeast zone of sinistral ductile shear caused by temporary locking of the southern segment of the Grenville Front boundary fault (now under Lake Huron).All structural facts can be explained without large differential translations of crustal slices. For example, most discordances in the regional gneissosity pattern could have been created by décollement and repeated buckling. Detailed geobarometry and petrologic studies may be required to settle the question of large-scale thrusting within the Grenville gneiss terrane.


1977 ◽  
Vol 14 (8) ◽  
pp. 1708-1720 ◽  
Author(s):  
S. G. Themistocleous ◽  
W. M. Schwerdtner

The Grenville Front Tectonic Zone extends as much as 30 km into the Grenville Province of Ontario, but reaches only a few kilometres into the Superior and Southern Provinces. For a distance of >75 km, this tectonic zone passes through a large granitic body, the Ingall Lake Batholith. Here the Superior portion of the zone is characterized by numerous north to northeast trending faults which cut the Grenville Front Boundary Fault. One of these younger structures, the Kettle Lake Fault, is exposed on Highway 11 about 1 km north of the Grenville Front Boundary Fault. Its mylonites are generally derived from feldspar-porphyritic trondhjemite, and contain numerous folded dykes of pink aplite.The folds plot into J. G. Ramsay's class 1C field, and represent flattened buckles. Using Ramsay's methods, C/B (flattening) and C (buckling) were estimated for the preserved parts of seven minor folds. The remaining components of overall strain were calculated on the basis of k-values obtained for the mylonitic trondhjemite adjacent to the buckles. Susceptibility anisotropy determinations provided an objective but minimal measure of k. The dilatational part of the deformation was ignored by putting ABC = 1. Thus for B (buckling) we found that B3 − B2C(1 −(1/k)) − 1/k = 0. This cubic equation has one real root B and two conjugate imaginary roots. Similarly for the flattening phase, A/B = 1 − k(1 − (B/C). Total strain components were obtained by superimposing the flattening strain on the buckling strain. Maximum values of C range from 0.081 to 0.395 depending on the severity of mylonitization.


2008 ◽  
Vol 113 (A9) ◽  
pp. n/a-n/a ◽  
Author(s):  
Charles J. Farrugia ◽  
Nikolai V. Erkaev ◽  
Ulrich Taubenschuss ◽  
Vladimir A. Shaidurov ◽  
Charles W. Smith ◽  
...  

2007 ◽  
Vol 25 (12) ◽  
pp. 2641-2648 ◽  
Author(s):  
R. P. Lepping ◽  
T. W. Narock ◽  
H. Chen

Abstract. We investigate the ability of the cylindrically symmetric force-free magnetic cloud (MC) fitting model of Lepping et al. (1990) to faithfully reproduce actual magnetic field observations by examining two quantities: (1) a difference angle, called β, i.e., the angle between the direction of the observed magnetic field (Bobs) and the derived force free model field (Bmod) and (2) the difference in magnitudes between the observed and modeled fields, i.e., ΔB(=|Bobs|−|Bmod|), and a normalized ΔB (i.e., ΔB/<B>) is also examined, all for a judiciously chosen set of 50 WIND interplanetary MCs, based on quality considerations. These three quantities are developed as a percent of MC duration and averaged over this set of MCs to obtain average profiles. It is found that, although and its normalize version are significantly enhanced (from a broad central average value) early in an average MC (and to a lesser extent also late in the MC), the angle is small (less than 8°) and approximately constant all throughout the MC. The field intensity enhancements are due mainly to interaction of the MC with the surrounding solar wind plasma causing field compression at front and rear. For example, for a typical MC, ΔB/ is: 0.21±0.27 very early in the MC, −0.11±0.10 at the center (and −0.085±0.12 averaged over the full "central region," i.e., for 30% to 80% of duration), and 0.05±0.29 very late in the MC, showing a double sign change as we travel from front to center to back, in the MC. When individual MCs are examined we find that over 80% of them possess field enhancements within several to many hours of the front boundary, but only about 30% show such enhancements at their rear portions. The enhancement of the MC's front field is also due to MC expansion, but this is usually a lesser effect compared to compression. It is expected that this compression is manifested as significant distortion to the MC's cross-section from the ideal circle, first suggested by Crooker et al. (1990), into a more elliptical/oval shape, as some global MC studies seem to confirm (e.g., Riley and Crooker, 2004) and apparently also as confirmed for local studies of MCs (e.g., Hidalgo et al., 2002; Nieves-Chinchilla et al., 2005).


2018 ◽  
Author(s):  
Chen Zhao ◽  
Rupert M. Gladstone ◽  
Roland C. Warner ◽  
Matt A. King ◽  
Thomas Zwinger

Abstract. Many glaciers in West Antarctica and the Antarctic Peninsula are now rapidly losing ice mass. Understanding of the dynamics of these fast-flowing glaciers, and their potential future behavior, can be improved through ice sheet modeling studies. Inverse methods are commonly used in ice sheet models to infer the basal shear stress, which has a large effect on the basal velocity and internal ice deformation. Here we use the full-Stokes Elmer/Ice model to simulate the Wordie Ice Shelf-Fleming Glacier system in the southern Antarctic Peninsula. With a control inverse method, we model the basal drag from the surface velocities observed in 2008. We propose a three-cycle spin-up scheme to remove the influence of initial temperature field on the final inversion. This is particularly important for glaciers with significant temperature-dependent internal deformation. We find that the Fleming Glacier has strong, temperature-dependent, deformational flow in the fast-flowing regions. Sensitivity tests using various bed elevation datasets and ice front boundary conditions demonstrate the importance of high-accuracy ice thickness/bed geometry data and precise location of the ice front boundary.


2018 ◽  
Vol 12 (8) ◽  
pp. 2637-2652 ◽  
Author(s):  
Chen Zhao ◽  
Rupert M. Gladstone ◽  
Roland C. Warner ◽  
Matt A. King ◽  
Thomas Zwinger ◽  
...  

Abstract. Many glaciers in the Antarctic Peninsula are now rapidly losing mass. Understanding of the dynamics of these fast-flowing glaciers, and their potential future behaviour, can be improved through ice sheet modelling studies. Inverse methods are commonly used in ice sheet models to infer the spatial distribution of a basal friction coefficient, which has a large effect on the basal velocity and ice deformation. Here we use the full-Stokes Elmer/Ice model to simulate the Wordie Ice Shelf–Fleming Glacier system in the southern Antarctic Peninsula. With an inverse method, we infer the pattern of the basal friction coefficient from surface velocities observed in 2008. We propose a multi-cycle spin-up scheme to reduce the influence of the assumed initial englacial temperature field on the final inversion. This is particularly important for glaciers like the Fleming Glacier, which have areas of strongly temperature-dependent deformational flow in the fast-flowing regions. Sensitivity tests using various bed elevation datasets, ice front positions and boundary conditions demonstrate the importance of high-accuracy ice thickness/bed geometry data and precise location of the ice front boundary.


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