我正在嘗試在 IEEE 交易論文中放置一個表格,該表格非常長並且將跨越兩頁。但我無法使用我正在使用的當前軟體包來做到這一點:任何建議都會非常有幫助。
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\begin{table*}[t!]
\centering
\caption{Comparison of SDP and BFM-SOCP based relaxation for multi-phase Active DNNs for $R_{gnd}=1\Omega$}
\scriptsize
\renewcommand{\arraystretch}{1.3}
\begin{tabular}{|c||c|c|c|c|c||c|c|c|c|c||c|c|c|c|c|}
\hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{OF:1 Slack Bus Power (kVA)}}\\ \hline
\multirow{6}{*}{\textbf{LMs}}&\multicolumn{5}{c||}{\textit{Y-connected End-Users}}&\multicolumn{5}{c||}{\textit{$\Delta$-connected End-Users}}&\multicolumn{5}{c|}{\textit{Y-$\Delta$ connected End-Users}}\\ \cline{2-16}
&\multicolumn{2}{c|}{\textbf{SDP}}&\multicolumn{3}{c||}{\textbf{BFM-SOCP}}&\multicolumn{2}{c|}{\textbf{SDP}}&\multicolumn{3}{c||}{\textbf{BFM-SOCP}}&\multicolumn{2}{c|}{\textbf{SDP}}&\multicolumn{3}{c|}{\textbf{BFM-SOCP}}\\ \cline{2-16}
&{\thead{\textit{EVR} \\ $|\lambda_2|/|\lambda_1|$\\ $\times 10^{-5}$}}&{\thead{\textit{Obj.}\\\textit{Value}}}&\multicolumn{3}{c||}{\textit{\% Optimality Gap}}&{\thead{\textit{EVR} \\ $|\lambda_2|/|\lambda_1|$\\ $\times 10^{-5}$}}&{\thead{\textit{Obj.}\\\textit{Value}}}&\multicolumn{3}{c||}{\textit{\% Optimality Gap}}&{\thead{\textit{EVR} \\ $|\lambda_2|/|\lambda_1|$\\ $\times 10^{-5}$}}&{\thead{\textit{Obj.}\\\textit{Value}}}&\multicolumn{3}{c|}{\textit{\% Optimality Gap}} \\ \hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{MicroGrid: Lightly Unbalanced DN}}\\ \hline
\textbf{LM:1}&0.32&2826.2&0.00&0.00 &0.00 & 2.86 & 2810.1 & 0.57 & 0.57 & 0.58 & 1.12 & 2829.5 & 0.16 & 0.16 & 0.16\\\hline
\textbf{LM:2}&0.15&2917.4&\textbf{4.33}&\textbf{12.2} &\textit{0.10} & 0.72 & 2917.6 & \textbf{4.34} & \textbf{12.2} & \textit{0.09} & 1.65 & 2906.2 & \textbf{4.33} & \textbf{11.8} & \textit{0.50}\\\hline
\textbf{LM:3}&0.16&3019.7&0.04&0.04 &0.04 & 1.18 & 3027.2 & 0.21 & 0.21 & 0.20 & 0.17 & 3021.8 & 0.06 & 0.06 & 0.06\\\hline
\textbf{LM:4}&0.30&2881.0&0.04&0.04 &0.39 & 0.05 & 2882.7 & 0.10 & 0.10 & 0.45 & \textbf{55.2} & 3131.1 & 0.45 & 0.09 & 1.34\\\hline
\textbf{LM:5}&0.15&2927.8&0.02&0.02 &0.01 & 2.26 & 2940.4 & 0.41 & 0.41 & 0.42 & 0.17 & 2928.8 & 0.01 & 0.01 & 0.00\\\hline
\textbf{LM:6}&0.28&2918.5&0.03&0.03 &0.15 & 0.15 & 2920.9 & 0.05 & 0.05 & 0.23 & 0.40 & 2943.6 & 0.01 & 0.03 & 0.31\\\hline
\textbf{LM:7}&0.04&2943.8&0.01&0.01 &0.10 & 0.16 & 2942.9 & 0.02 & 0.02 & 0.07 & 1.53 & 2944.2 & 0.03 & 0.03 & 0.06\\\hline
\textbf{LM:8}&1.27&2953.6&0.24&0.24 &0.24 & 0.11 & 2946.0 & 0.02 & 0.02 & 0.02 & 0.28 & 2944.7 & 0.09 & 0.09 & 0.09\\\hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{IT-37: Moderately Unbalanced DN}}\\
\textbf{LM:1}&0.34 &97.7 &0.15&0.15& 0.15& 0.11& 98.0 & 0.01 & 0.01 & 0.01 & 0.47 & 97.4 & 0.03 & 0.03 & 0.03\\\hline
\textbf{LM:2}&1.34 &100.7&\textbf{6.13}&\textbf{13.7}& \textit{0.23}& 0.28& 100.7 & \textbf{6.02} & \textbf{13.8} & \textit{0.21} & 0.93 & 100.6 & \textbf{6.62} & \textbf{13.52} & \textit{0.27}\\\hline
\textbf{LM:3}&0.84 &104.0&0.14&0.14& 0.14& 0.51& 103.9 & 0.13 & 0.13 & 0.13 & 0.48 & 104.2 & 0.30 & 0.30 & 0.30\\\hline
\textbf{LM:4}&1.96 &98.4 &0.66&0.66& 0.88& 1.87& 112.9 & \textit{0.51} & \textit{0.18} & \textbf{1.67} & \textbf{110} & 122.3 & 1.53 & 3.28 & 4.79\\\hline
\textbf{LM:5}&0.56 &101.0&0.18&0.18& 0.17& 0.46& 101.2 & 0.00 & 0.00 & 0.01 & 0.53 & 101.0 & 0.14 & 0.14 & 0.13\\\hline
\textbf{LM:6}&1.47 &100.3&0.33&0.33& 0.35& 0.36& 102.9 & 0.23 & 0.27 & 0.45 & 0.93 & 102.8 & 0.51 & 0.33 & 0.01\\\hline
\textbf{LM:7}&0.44 &101.1&0.34&0.34& 0.37& 0.18& 101.5 & 0.12 & 0.12 & 0.05 & 0.28 & 101.4 & 0.04 & 0.03 & 0.07\\\hline
\textbf{LM:8}&0.66 &101.6&0.25&0.25& 0.25& 0.15& 101.8 & 0.04 & 0.04 & 0.04 & 0.34 & 101.8 & 0.14 & 0.14 & 0.14\\\hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{Cigre: Highly Unbalanced DN}}\\
\textbf{LM:1}&1.09&146.4&0.07&0.07& 0.07& 1.58& 146.7 & 0.04 & 0.04 & 0.04 & 0.93 & 146.6 & 0.03 & 0.03 & 0.03\\\hline
\textbf{LM:2}&1.02&153.8&\textbf{10.8}&\textbf{21.1}& \textit{0.16}& 1.39& 153.9 & \textbf{9.14} & \textbf{20.9} & \textit{0.18} & 0.90 & 153.8 & \textbf{10.12} & \textbf{20.9} &\textit{0.19}\\\hline
\textbf{LM:3}&0.72&162.7&0.00&0.00& 0.00& 0.92& 162.8 & 0.02 & 0.02 & 0.02 & 1.27 & 162.8 & 0.05 & 0.05 & 0.05\\\hline
\textbf{LM:4}&\textbf{13.1}&150.0&0.01&7.63& 8.68& \textbf{1680}& 194.3 & 0.84 & 29.9 & 31.9 & \textbf{120} & 160.7 & 1.04 & 11.8 & 13.1\\\hline
\textbf{LM:5}&0.77&154.8&0.01&0.01& 0.02& 0.78& 155.1 & 0.00 & 0.00 & 0.05 & 1.25 & 154.9 & 0.03 & 0.03 & 0.00\\\hline
\textbf{LM:6}&7.03&154.0&0.03&0.10& 0.59& \textbf{63.3}& 167.5 & 1.65 & 0.81 & 2.89 & 4.44 & 156.4 & 1.02 & 0.59 & 0.77\\\hline
\textbf{LM:7}&3.11&156.1&0.00&0.02& 0.23& 1.93& 157.1 & \textbf{1.19} & \textbf{1.04} & \textit{0.35} & 2.21 & 156.5 & 0.02 & 0.03 & 0.24\\\hline
\textbf{LM:8}&0.82&156.3&0.01&0.01& 0.01& 1.52& 156.5 & 0.02 & 0.02 & 0.02 & 1.18 & 156.4 & 0.03 & 0.03 & 0.03\\\hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{IEEE-13: Highly Unbalanced DN}}\\
\textbf{LM:1}&0.66&3620.4&0.17&0.17 &0.17 & 3.17& 3623.5 & 0.75 & 0.75 & 0.76 & 1.17 & 3611.7 & 0.42 & 0.42 & 0.43\\\hline
\textbf{LM:2}&0.54&3810.3&\textbf{12.7}&\textbf{21.7} &\textit{0.34} & 4.91& 3796.8 & \textbf{10.0} & \textbf{19.9} & \textit{0.46} & 1.69 & 3808.2 & \textbf{13.3} & \textbf{22.1} & \textit{0.40}\\\hline
\textbf{LM:3}&1.50&4033.6&0.40&0.40 &0.40 & 0.74& 3991.5 & 0.06 & 0.06 & 0.06 & 2.21 & 4062.8 & 0.23 & 0.23 & 0.23\\\hline
\textbf{LM:4}&3.26&3639.6&\textbf{2.45}&\textbf{8.02} &\textit{0.79} & \textbf{5870}& 8535.5 & 9.65 & 24.5 & 5.34 & 2.79 & 3932.1 & \textbf{2.48} & \textbf{4.54} & \textit{0.56}\\\hline
\textbf{LM:5}&1.36&3825.8&0.39&0.30 &0.39 & 0.53& 3830.1 & 0.05 & 0.05 & 0.06 & 2.02 & 3877.3 & 0.84 & 0.94 & 0.86\\\hline
\textbf{LM:6}&1.14&3777.7&0.10&0.10 &0.61 & \textbf{170} & 1265.9 & 3.86 & 5.00 & 0.05 & 3.78 & 3799.0 & \textbf{2.24} & \textbf{3.01} & \textit{0.66}\\\hline
\textbf{LM:7}&1.34&3852.9&0.05&0.66 &0.32 & 0.40& 3868.5 & 0.14 & 0.18 & 0.24 & 1.15 & 3859.5 & 0.18 & 0.50 & 0.02\\\hline
\textbf{LM:8}&4.89&3891.4&0.86&0.86 &0.87 & 0.14& 3865.0 & 0.01 & 0.01 & 0.01 & 3.84 & 3878.8 & 0.47 & 0.47 & 0.47\\\hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{IEEE-13: Highly Unbalanced DN}}\\
\textbf{LM:1}&0.66&3620.4&0.17&0.17 &0.17 & 3.17& 3623.5 & 0.75 & 0.75 & 0.76 & 1.17 & 3611.7 & 0.42 & 0.42 & 0.43\\\hline
\textbf{LM:2}&0.54&3810.3&\textbf{12.7}&\textbf{21.7} &\textit{0.34} & 4.91& 3796.8 & \textbf{10.0} & \textbf{19.9} & \textit{0.46} & 1.69 & 3808.2 & \textbf{13.3} & \textbf{22.1} & \textit{0.40}\\\hline
\textbf{LM:3}&1.50&4033.6&0.40&0.40 &0.40 & 0.74& 3991.5 & 0.06 & 0.06 & 0.06 & 2.21 & 4062.8 & 0.23 & 0.23 & 0.23\\\hline
\textbf{LM:4}&3.26&3639.6&\textbf{2.45}&\textbf{8.02} &\textit{0.79} & \textbf{5870}& 8535.5 & 9.65 & 24.5 & 5.34 & 2.79 & 3932.1 & \textbf{2.48} & \textbf{4.54} & \textit{0.56}\\\hline
\textbf{LM:5}&1.36&3825.8&0.39&0.30 &0.39 & 0.53& 3830.1 & 0.05 & 0.05 & 0.06 & 2.02 & 3877.3 & 0.84 & 0.94 & 0.86\\\hline
\textbf{LM:6}&1.14&3777.7&0.10&0.10 &0.61 & \textbf{170} & 1265.9 & 3.86 & 5.00 & 0.05 & 3.78 & 3799.0 & \textbf{2.24} & \textbf{3.01} & \textit{0.66}\\\hline
\textbf{LM:7}&1.34&3852.9&0.05&0.66 &0.32 & 0.40& 3868.5 & 0.14 & 0.18 & 0.24 & 1.15 & 3859.5 & 0.18 & 0.50 & 0.02\\\hline
\textbf{LM:8}&4.89&3891.4&0.86&0.86 &0.87 & 0.14& 3865.0 & 0.01 & 0.01 & 0.01 & 3.84 & 3878.8 & 0.47 & 0.47 & 0.47\\\hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{IEEE-13: Highly Unbalanced DN}}\\
\textbf{LM:1}&0.66&3620.4&0.17&0.17 &0.17 & 3.17& 3623.5 & 0.75 & 0.75 & 0.76 & 1.17 & 3611.7 & 0.42 & 0.42 & 0.43\\\hline
\textbf{LM:2}&0.54&3810.3&\textbf{12.7}&\textbf{21.7} &\textit{0.34} & 4.91& 3796.8 & \textbf{10.0} & \textbf{19.9} & \textit{0.46} & 1.69 & 3808.2 & \textbf{13.3} & \textbf{22.1} & \textit{0.40}\\\hline
\textbf{LM:3}&1.50&4033.6&0.40&0.40 &0.40 & 0.74& 3991.5 & 0.06 & 0.06 & 0.06 & 2.21 & 4062.8 & 0.23 & 0.23 & 0.23\\\hline
\textbf{LM:4}&3.26&3639.6&\textbf{2.45}&\textbf{8.02} &\textit{0.79} & \textbf{5870}& 8535.5 & 9.65 & 24.5 & 5.34 & 2.79 & 3932.1 & \textbf{2.48} & \textbf{4.54} & \textit{0.56}\\\hline
\textbf{LM:5}&1.36&3825.8&0.39&0.30 &0.39 & 0.53& 3830.1 & 0.05 & 0.05 & 0.06 & 2.02 & 3877.3 & 0.84 & 0.94 & 0.86\\\hline
\textbf{LM:6}&1.14&3777.7&0.10&0.10 &0.61 & \textbf{170} & 1265.9 & 3.86 & 5.00 & 0.05 & 3.78 & 3799.0 & \textbf{2.24} & \textbf{3.01} & \textit{0.66}\\\hline
\textbf{LM:7}&1.34&3852.9&0.05&0.66 &0.32 & 0.40& 3868.5 & 0.14 & 0.18 & 0.24 & 1.15 & 3859.5 & 0.18 & 0.50 & 0.02\\\hline
\textbf{LM:8}&4.89&3891.4&0.86&0.86 &0.87 & 0.14& 3865.0 & 0.01 & 0.01 & 0.01 & 3.84 & 3878.8 & 0.47 & 0.47 & 0.47\\\hline
\multicolumn{16}{|c|}{\cellcolor{gray!50}\textbf{IEEE-13: Highly Unbalanced DN}}\\
\textbf{LM:1}&0.66&3620.4&0.17&0.17 &0.17 & 3.17& 3623.5 & 0.75 & 0.75 & 0.76 & 1.17 & 3611.7 & 0.42 & 0.42 & 0.43\\\hline
\textbf{LM:2}&0.54&3810.3&\textbf{12.7}&\textbf{21.7} &\textit{0.34} & 4.91& 3796.8 & \textbf{10.0} & \textbf{19.9} & \textit{0.46} & 1.69 & 3808.2 & \textbf{13.3} & \textbf{22.1} & \textit{0.40}\\\hline
\textbf{LM:3}&1.50&4033.6&0.40&0.40 &0.40 & 0.74& 3991.5 & 0.06 & 0.06 & 0.06 & 2.21 & 4062.8 & 0.23 & 0.23 & 0.23\\\hline
\textbf{LM:4}&3.26&3639.6&\textbf{2.45}&\textbf{8.02} &\textit{0.79} & \textbf{5870}& 8535.5 & 9.65 & 24.5 & 5.34 & 2.79 & 3932.1 & \textbf{2.48} & \textbf{4.54} & \textit{0.56}\\\hline
\textbf{LM:5}&1.36&3825.8&0.39&0.30 &0.39 & 0.53& 3830.1 & 0.05 & 0.05 & 0.06 & 2.02 & 3877.3 & 0.84 & 0.94 & 0.86\\\hline
\textbf{LM:6}&1.14&3777.7&0.10&0.10 &0.61 & \textbf{170} & 1265.9 & 3.86 & 5.00 & 0.05 & 3.78 & 3799.0 & \textbf{2.24} & \textbf{3.01} & \textit{0.66}\\\hline
\textbf{LM:7}&1.34&3852.9&0.05&0.66 &0.32 & 0.40& 3868.5 & 0.14 & 0.18 & 0.24 & 1.15 & 3859.5 & 0.18 & 0.50 & 0.02\\\hline
\textbf{LM:8}&4.89&3891.4&0.86&0.86 &0.87 & 0.14& 3865.0 & 0.01 & 0.01 & 0.01 & 3.84 & 3878.8 & 0.47 & 0.47 & 0.47\\\hline
\end{tabular}
\begin{tablenotes}\scriptsize
\centering
\item LM: Load Model \hspace{0.2em} EVR: Eigen Value Ratio \hspace{0.2em} \hspace{0.2em} IT: Italian \hspace{0.2em} SDP: Semi-Definite Programming \hspace{0.2em} BFM-SOCP: Branch Flow Relaxation-Second Order Cone Programming
\end{tablenotes}
\label{Table_2}
\end{table*}
\end{document}