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Rock Mechanics.pdf - Mining and Blasting

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LONGWALL AND CAVING MINING METHODS<br />

(c) Using equation 10.84, calculate the mining-induced elastic displacements of the<br />

upper <strong>and</strong> lower surfaces at the midpoint of each of the excavations if G =<br />

16 GPa <strong>and</strong> = 0.20.<br />

2 A 1.0 m thick, flat-lying, metalliferous orebody of large areal extent is to be extracted<br />

by a longwall method. The in situ vertical stress at the mining depth is 85 MPa,<br />

<strong>and</strong> Young’s modulus <strong>and</strong> Poisson’s ratio of the rock are 48 GPa <strong>and</strong> 0.20, respectively.<br />

(a) Calculate the critical span of a longwall face under these conditions. What total<br />

amount of energy is released per unit length of stope <strong>and</strong> per unit volume of<br />

extraction, for this critical span? What values do these quantities approach as<br />

the span increases above the critical?<br />

(b) Partial extraction is to be used to control the energy release rates in this case.<br />

Using equations 10.88 <strong>and</strong> 15.1, write down an expression for the total energy<br />

released per unit volume of extraction when the orebody is mined in a number of<br />

parallel panels of span, l, spaced on centres of S as in Figure 15.5a. Determine<br />

values of l <strong>and</strong> S that will restrict this energy release rate to 15 MJ m −3 <strong>and</strong><br />

maintain an extraction ratio of at least 0.80. In order to ensure the long-term<br />

stability of the pillars it is necessary that they have width to height ratios of at<br />

least 20.<br />

3 A 2.5 m thick horizontal coal seam at a depth of 230 m is to be extracted by a<br />

series of parallel longwall panels with a single row of pillars between them as shown<br />

in Figure 15.7. The roadways are to be 4.5 m wide <strong>and</strong> the weighted unit weight of<br />

the overburden materials is = 25 kN m −3 . The distribution of vertical stress with<br />

distance, x, from the pillar rib side is of the type illustrated in Figure 15.9 with the<br />

width of the yield zone xb = 10 m <strong>and</strong> the peak stress yy = 12 MPa. The vertical<br />

stress, zz, decays with distance into the solid coal away from the yield zone according<br />

to the equation<br />

where v is the in situ vertical stress.<br />

482<br />

(zz − v) = (yy − v) exp{(xb − x)/12}

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