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A cube has sides of length \( L \). It is placed with one corner at the origin (refer to figure). The electric field is uniform and given by \( \vec{E}=-B i+C^{\prime} j-D k \), where \( B, C \), and \( D \) are positive constants. The flux passing through the different surfaces (match the table) is
\begin{tabular}{|l|l|}
\hline Surface & Flux \\
\hline (i) \( S_{1} \) & (m) \( B L^{2} \) \\
\hline (ii) \( S_{2} \) & (n) \( -B L^{2} \) \\
\hline (iii) \( S_{3} \) & (0) \( C L^{2} \) \\
\hline (iv) \( S_{4} \) & (p) \( -C L^{2} \) \\
\hline (v) \( S_{5} \) & (q) \( D L^{2} \) \\
\hline (vi) \( S_{6} \) & (r) \( -D L^{2} \) \\
\hline
\end{tabular}
(1) (i, p), (ii, r), (iii, o), (iv, q), (v, n), (vi, m)
(2) (i, r), (ii, p), (iii, q), (iv, n), (v, m), (vi, o)
(3) (i, m), (ii, n), (iii, o), (iv, p), (v, q), (vi, r)
(4) (i, r), (ii, q), (iii, p), (iv, o), (v, n), (vi, m)
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