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PERMFILE41761
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PERMFILE41761
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Last modified
8/24/2016 10:44:21 PM
Creation date
11/20/2007 10:53:14 AM
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Template:
DRMS Permit Index
Permit No
M1999002
IBM Index Class Name
Permit File
Doc Date
6/18/1999
Doc Name
OBJECTORS EXHIBITS
Media Type
D
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No
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Analytical Methods <br />along bedding planes are also applicable (or slippage along <br />other discontinuities. <br />DEVELOPi<1ENT AND PREL]iVIINARY <br />EVALUATION OF METHODS FOR <br />PREDICTING SUBSIDENCE <br />In this section, analytical methods for predicting sub- <br />sidence which include the capability of accounting for the <br />inability of rock to withstand tensile stresses and the possi- <br />bility of slippage along bedding planes are described. Ex- <br />amples were analyzed to determine the significance of <br />these phenomzna on the prediction of subsidence. <br />"No tension" analysis <br />When numerous cracks and fissurzs are present in a <br />rock mass, it has bzen assumed that the rock is incapable <br />of withstanding tensile stresses. A procedure for modell- <br />ingthis nonlinear behavior has been presented by Zienkie- <br />wicz, et al. (1968). This method, called "no tension" or <br />"stress transfer" analysis, consists of five essential sups: <br />(a) Assign initial stresses to the rock mass, and cal- <br />culate boundary loads rzquired on the cavity' (ace <br />to simulate the creation of the opening. <br />(b) Analyze the problem as an elastic case. Add the <br />induced changes in stress to the initial stresses <br />and compute the principal stresses. <br />(c) Determine elements in which tension exists. As <br />thz material is assumed incapable of sustaining <br />tensions, the calculated tensile principal stresses <br />are eliminated without permitting any point in <br />[he structure to displace. In order to maintain <br />equilibrium, external equivalent nodal point <br />forces are calculated and temporarily applied to <br />the structure. <br />(d) The elastic analysis is repeated to remocz the <br />balancing nods! point forces and the check for <br />tensiiz stresses is repeated. <br />(e) If, at thz end of stags (d). [ht tznsih principal <br />stresses are still in zxistenci, steps (c) and (d)art <br />repeated until all tensile stresses are reduced to <br />an acceptable level. <br />In Step (c), when the linear elastic solution indicates that <br />the rock is subjected to [ensile stresses greatzr than the <br />tensile strength, the rock is assumed to be fractured and <br />incapable oftransferring stresses between two orthogonal <br />directions. To include this effect, a correction has to be <br />made on the stress before the stress transfer process is <br />performed. In the case where both principal tensile <br />stresses v,' and oy' are to be transferred, the "correctzd" <br />stresses are given by <br /> <br />• 105 <br /> <br />Slippage along bedding planes <br />Gadding plants are likely to be present in szdimentary <br />rocks in which thz majority of the solution and coal min- <br />ing is carried out, Shear strength along bidding planes is <br />considered to be weaker than that of intact rocks. As the <br />shear stress overcomes thz shear strength along these <br />planes dui to chanees in stress induced by thz creation of <br />underground cavities, slippage may occur along these rock <br />beds. This type of behavior may causz changes in the <br />subsidence profile calculated by the elastic analysis of the <br />underground cavity assuming the rock to bz a continuum. <br />The two major di.bcultizs of incorporating this aspect of <br />rock behavior into an analytical modzl for predicting field <br />trzhavior are (1) thz detzrntination of thz number and <br />location of thz bedding planes, and (2) chi representation <br />of thz behavior of [hzse bedding plants, i.e., assigning the <br />stress-strain behavior and the strength of these weak <br />planes. The numbzr and location of the weak planes may <br />be approximately estimated from 3-D velocity logs [akin <br />in the mined areas. It is, however, difficult to determine <br />the stress-strain behavior of these bedding plants. As a <br />first step to study the effects of the presettcz of the weak <br />beddine planes in the rock mass above the cavity on thz <br />subsidence profile, it is assumed in this study that [hest <br />bedding plants werz eery weak in resisting shear stress <br />along the bedding planes and would yizld upon creation <br />of an opening. <br />Illustrative problem <br />A rock profile with the sizz and I~xation of the cavity <br />shown in Figure 4 was analyzed [o studs the effects of <br />no-tension rock characteristics and the presence of bzd- <br />ding plants on the subsidence profile. Thrze weak bedding <br />planes were assumed, and their locations art shown in <br />Figure -i. Thzsz weak plants were assiened to a very low <br />shear modulus and. therefore, oRzrzd very li[tlz rzsistance <br />to movzmzn[ along the plant. Thz result of the analysis <br />indicates that the vertical subsidence at the cznterlini of <br />the cavity is thrze times as large as the calculated without <br />[he presence of thz bidding plants. Furthermore, thz <br />shape of the subsidence profile indicates a greater localiza- <br />tion of [he subsidence to an aria about the cavity than for <br />the elastic continuum case. This shapz is in general agree- <br />ment with that observed in the field. The subsidence pro- <br />file obtained from the analysis is presented in Figure 5. <br />The results of the analysis indicate that the presence of <br />weak bidding plants above the cavity has a major effect <br />on thz magnitude and distribution of the subsidence. It <br />may be noted that a "no-tension"' analysis, i.z., assuming <br />that the rock mass in its natural state is incapable of <br />sustaining tensile stresses, provides a slight increase in <br />subsidence. <br />
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