# Detecting Atypical Values and Their Influence on Blast-Induced Seismic Measurement Results
## 3 Results
\begin{table}
\begin{tabular}{c c c c c} \hline
**Borehole** & **Conf. Int. (\%)** & **95\%-Line Equation** & **R\({}^{2}\)** & **Std. Dev.** \\ \hline \multirow{3}{*}{B1} & 68.27 & V = 880.5 \(\times\) (SD)\({}^{-1.421}\) & 0.997 & 0.027 \\  & 95.45 & V = 977.2 \(\times\) (SD)\({}^{-1.450}\) & 0.988 & 0.051 \\  & 100.00 & V = 1160.07 \(\times\) (SD)\({}^{-1.403}\) & 0.952 & 0.096 \\ \hline \multirow{3}{*}{B2} & 68.27 & / & / & / \\  & 95.45 & V = 746.9 \(\times\) (SD)\({}^{-1.174}\) & 0.774 & 0.156 \\  & 100.00 & V = 731.2 \(\times\) (SD)\({}^{-1.117}\) & 0.703 & 0.167 \\ \hline \multirow{3}{*}{B3} & 68.27 & / & / & / \\  & 95.45 & V = 608.9 \(\times\) (SD)\({}^{-1.160}\) & 0.927 & 0.064 \\  & 100.00 & V = 487.5 \(\times\) (SD)\({}^{-0.897}\) & 0.624 & 0.138 \\ \hline \multirow{3}{*}{B4} & 68.27 & / & / & / \\  & 95.45 & V = 322.9 \(\times\) (SD)\({}^{-0.923}\) & 0.732 & 0.122 \\  & 100.00 & V = 270.6 \(\times\) (SD)\({}^{-0.737}\) & 0.423 & 0.180 \\ \hline \multirow{3}{*}{B5} & 68.27 & V = 65.65 \(\times\) (SD)\({}^{-0.431}\) & 0.369 & 0.099 \\  & 95.45 & V = 77.01 \(\times\) (SD)\({}^{-0.506}\) & 0.466 & 0.095 \\  & 100.00 & V = 60.71 \(\times\) (SD)\({}^{-0.300}\) & 0.086 & 0.165 \\ \hline \multirow{3}{*}{B6} & 68.27 & / & / & / \\  & 95.45 & V = 624.5 \(\times\) (SD)\({}^{-1.214}\) & 0.997 & 0.019 \\  & 95.45 & V = 659.2 \(\times\) (SD)\({}^{-1.233}\) & 0.995 & 0.027 \\  & 100.00 & V = 776.4 \(\times\) (SD)\({}^{-1.251}\) & 0.984 & 0.046 \\ \hline \multirow{3}{*}{B7} & 68.27 & / & / & / \\  & 95.45 & V = 133.4 \(\times\) (SD)\({}^{-0.610}\) & 0.780 & 0.064 \\  & 100.00 & V = 293.6 \(\times\) (SD)\({}^{-0.883}\) & 0.713 & 0.113 \\ \hline \multirow{3}{*}{B8} & 68.27 & / & / & / \\  & 95.45 & V = 876.8 \(\times\) (SD)\({}^{-1.184}\) & 0.785 & 0.105 \\  & 100.00 & V = 876.8 \(\times\) (SD)\({}^{-1.184}\) & 0.785 & 0.105 \\ \hline \multirow{3}{*}{B9} & 68.27 & V = 346.6 \(\times\) (SD)\({}^{-1.079}\) & 0.985 & 0.043 \\  & 95.45 & V = 384.1 \(\times\) (SD)\({}^{-1.097}\) & 0.979 & 0.049 \\  & 100.00 & V = 889.8 \(\times\) (SD)\({}^{-1.272}\) & 0.878 & 0.135 \\ \hline \multirow{3}{*}{B10} & 68.27 & V = 75.77 \(\times\) (SD)\({}^{-0.683}\) & 0.997 & 0.009 \\  & 95.45 & V = 64.00 \(\times\) (SD)\({}^{-0.525}\) & 0.799 & 0.062 \\  & 100.00 & V = 98.20 \(\times\) (SD)\({}^{-0.612}\) & 0.618 & 0.101 \\ \hline \multirow{3}{*}{B11} & 68.27 & V = 193.5 \(\times\) (SD)\({}^{-0.841}\) & 0.962 & 0.033 \\  & 95.45 & V = 178.5 \(\times\) (SD)\({}^{-0.791}\) & 0.926 & 0.042 \\  & 100.00 & V = 257.9 \(\times\) (SD)\({}^{-0.870}\) & 0.815 & 0.070 \\ \hline \multirow{3}{*}{B12} & 68.27 & V = 1237.4 \(\times\) (SD)\({}^{-1.551}\) & 0.986 & 0.062 \\  & 95.45 & V = 1035.2 \(\times\) (SD)\({}^{-1.442}\) & 0.917 & 0.128 \\  & 100.00 & V = 1357.4 \(\times\) (SD)\({}^{-1.381}\) & 0.791 & 0.195 \\ \hline \multirow{3}{*}{B13} & 68.27 & V = 1098.2 \(\times\) (SD)\({}^{-1.578}\) & 0.976 & 0.072 \\  & 95.45 & V = 1126.6 \(\times\) (SD)\({}^{-1.609}\) & 0.970 & 0.070 \\  & 100.00 & V = 2632.1 \(\times\) (SD)\({}^{-1.497}\) & 0.606 & 0.277 \\ \hline \multirow{3}{*}{B14} & 68.27 & V = 1283.3 \(\times\) (SD)\({}^{-1.647}\) & 0.953 & 0.083 \\  & 95.45 & V = 1446.4 \(\times\) (SD)\({}^{-1.694}\) & 0.949 & 0.083 \\  & 100.00 & V = 3075.3 \(\times\) (SD)\({}^{-1.581}\) & 0.565 & 0.274 \\ \hline \multirow{3}{*}{B15} & 68.27 & V = 1241.5 \(\times\) (SD)\({}^{-1.729}\) & 0.971 & 0.058 \\  & 95.45 & V = 1032.5 \(\times\) (SD)\({}^{-1.601}\) & 0.951 & 0.067 \\  & 100.00 & V = 1968.4 \(\times\) (SD)\({}^{-1.778}\) & 0.836 & 0.138 \\ \hline \multirow{3}{*}{B16} & 68.27 & V = 540.3 \(\times\) (SD)\({}^{-1.440}\) & 0.990 & 0.038 \\  & 95.45 & V = 554.1 \(\times\) (SD)\({}^{-1.236}\) & 0.902 & 0.109 \\  & 100.00 & V = 1015.1 \(\times\) (SD)\({}^{-1.400}\) & 0.751 & 0.203 \\ \hline \multirow{3}{*}{B17} & 68.27 & / & / & / \\  & 95.45 & V = 778.8 \(\times\) (SD)\({}^{-1.052}\) & 0.806 & 0.183 \\ \hline \end{tabular}
\end{table}