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首页> 外文期刊>資源と素材: 资源·素材学会志 >The Relationship Between the Shape of a Disced Core and Three-Dimensional in-Situ Stresses Estimated by a Tensile Principal Stress Analysis
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The Relationship Between the Shape of a Disced Core and Three-Dimensional in-Situ Stresses Estimated by a Tensile Principal Stress Analysis

机译:圆盘形芯的形状与通过拉伸主应力分析估计的三维原位应力之间的关系

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Based upon the assumption that core discing results from tensile stresses within and below a core during boring, the direction of the principal tensile stress was analyzed in detail for the stress conditions where core discing is likely to occur to investigate the relationship between the shape of a disced core and in-situ stresses for the case of a long disced core. Main results obtained in this study are summarized as follows:1) In the central parts of the end surfaces, a relatively flat plane is formed. The azimuth of the normal direction of the plane coincides with that of the minimum principal stress, #sigma#_3. The inclination, #phi#_m of the normal direction from the core axis is approximately one thirds of that, #phi#_3 of #sigma#_3. By using the two equations, (1) and (3). a method for estimating more accurate #phi#_3 (+- 23 percent) was proposed.2) By combining the additional equation, (1) on the magnitudes of #sigma#_3, the mean stress, #sigma#_m and the stress in the direction of the core axis, #sigma#_Z with the previously proposed equation, (2), which is the condition of core discing, two of the above stresses can be determined if #phi#_m is measured and if one of them is determined independently. For the vertical borehole, by assuming #sigma#_Z to be an overburden pressure, #sigma#_m and #sigma#_3 can be determined from the two equations.3) When the difference between the maximum principal stress, #sigma#_1 and the intermediate principal stress, #sigma#_2 is large enough, a saddle shaped disc is formed and the shape becomes more distinct with the difference. For the upper end surface of the disced core, the azimuth of the concave upwards is approximately that of #sigma#_1 and that of convex upwards is approximately that of #sigma#_2. However, this does not hold strictly except the special stress conditions.4) When the difference between #sigma#_1 and #sigma#_2 is small, the disced core has almost flat end surfaces.5) The symmetry in the shape of a disced core coincides with that of in-situ stresses with respect to the axes on the core.6) A method was proposed to estimate all of the directions of the principal stresses from the symmetry of the disc shape. the normal direction of the central plane and the azimuth of the concave axis or the convex axis when one of the principal stresses is in one of the directions of the core axis and the axes perpendicular to the core axis.
机译:基于钻孔过程中岩心盘是由岩心内部和下方的拉应力产生的假设,针对可能发生岩心盘的应力条件,详细分析了主要拉应力的方向,以研究岩心形状之间的关系。盘状核和长形盘状核的原位应力。本研究获得的主要结果概括如下:1)在端面的中心部分,形成了相对平坦的平面。平面法线方向的方位角与最小主应力#sigma#_3的方位角重合。从芯轴开始的法线方向的倾斜度#phi#_m约为#sigma#_3的倾斜度#phi#_3的三分之一。通过使用两个等式(1)和(3)。提出了一种估计更准确的#phi#_3(+-23%)的方法。2)通过结合附加公式(1)来计算#sigma#_3的大小,平均应力,#sigma#_m和应力在芯轴的条件下,在芯轴方向#sigma#_Z与先前提出的方程式(2)中,如果测量了#phi#_m且其中之一,则可以确定上述两个应力是独立确定的。对于垂直井眼,通过将#sigma#_Z设为上覆压力,可以从两个等式确定#sigma#_m和#sigma#_3。3)当最大主应力,#sigma#_1和中间主应力#sigma#_2足够大,形成了鞍形圆盘,并且形状随着差异而变得更加明显。对于盘状芯的上端面,向上凹入的方位角大约是#sigma#_1的方位角,而向上凸出的方位角大约是#sigma#_2的方位角。但是,除特殊的应力条件外,这并不严格。4)#sigma#_1与#sigma#_2之差较小时,碟形磁芯的端面几乎平坦。5)碟形的对称性6)提出了一种根据圆盘形状的对称性来估算主应力所有方向的方法。当主应力之一在芯轴方向和垂直于芯轴的轴之一时,中心平面的法线方向和凹轴或凸轴的方位角。

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