Electronic Science and Technology ›› 2022, Vol. 35 ›› Issue (10): 65-71.doi: 10.16180/j.cnki.issn1007-7820.2022.10.011
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LIU Weixing,YANG Jinxian
Received:
2021-04-08
Online:
2022-10-15
Published:
2022-10-25
Supported by:
CLC Number:
LIU Weixing,YANG Jinxian. Pattern Recognition and Segmentation Method of Wellbore Trajectory Based on Characteristic Parameters[J].Electronic Science and Technology, 2022, 35(10): 65-71.
Table 1.
Basic parameters of trajectory"
测点数据 | 基本轨迹参数 | |||||
---|---|---|---|---|---|---|
井深 /m | 井斜角 /(°)·m-1 | 方位角 /(°)·m-1 | 井斜变化率 /(°)·m-1 | 方位变化率 /(°)·m-1 | 曲率 /(°)·m-1 | 挠率 /(°)·m-1 |
100 | 30.00 | 45.000 | - | - | - | - |
130 | 41.42 | 46.210 | 21.51 | 21.33 | 28.35 | 8.23 |
160 | 43.73 | 47.560 | 20.34 | 22.23 | 14.60 | 4.68 |
190 | 47.86 | 49.540 | 19.89 | 23.44 | 16.08 | 3.66 |
210 | 47.74 | 48.340 | 19.15 | 22.62 | 25.96 | 2.99 |
240 | 48.17 | 50.540 | 20.51 | 22.65 | 18.67 | 1.80 |
270 | 46.79 | 51.640 | 8.22 | 18.58 | 26.16 | 0.79 |
300 | 48.48 | 49.330 | 7.33 | 20.78 | 24.12 | 0.62 |
330 | 51.23 | 51.230 | 6.23 | 25.35 | 25.12 | 0.80 |
360 | 53.78 | 54.450 | 9.33 | 30.99 | 24.80 | 0.55 |
400 | 56.12 | 58.000 | 11.22 | 24.13 | 26.16 | 0.18 |
Table 2.
Average values and standard deviations of parameters"
井深 /m | 井斜角变化率 | 方位角变化率 | 曲率 | 挠率 | |||||
---|---|---|---|---|---|---|---|---|---|
平均值 | 方差 | 平均值 | 方差 | 平均值 | 方差 | 平均值 | 方差 | ||
130 | 21.51 | - | 21.33 | - | 28.350 0 | - | 8.230 | - | |
160 | 20.92 | 0.59 | 21.78 | 0.59 | 21.475 0 | 6.88 | 6.455 | 1.78 | |
190 | 20.58 | 0.68 | 22.33 | 0.68 | 19.670 0 | 6.16 | 5.520 | 1.96 | |
210 | 20.22 | 0.86 | 22.40 | 0.86 | 21.247 5 | 5.99 | 4.890 | 2.02 | |
240 | 20.28 | 0.77 | 22.45 | 0.77 | 20.732 0 | 5.46 | 0.272 | 2.19 | |
270 | 18.27 | 4.55 | 21.80 | 4.55 | 21.660 0 | 5.38 | 0.690 | 2.38 | |
300 | 16.70 | 5.69 | 21.66 | 5.69 | 21.990 0 | 5.05 | 0.250 | 2.45 | |
330 | 15.39 | 6.35 | 22.12 | 6.35 | 22.380 0 | 4.84 | 0.940 | 2.43 | |
360 | 14.72 | 6.29 | 23.10 | 6.29 | 22.650 0 | 4.62 | 0.680 | 2.42 | |
400 | 10.37 | 6.05 | 23.21 | 6.05 | 23.000 0 | 4.51 | 0.430 | 2.41 |
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