A conducting square loop of tabular |l|l|l| 3 |c| ⊗ & ⊗ல & QO & & － 00 808 & & ⊕ & & ✓ 86…

A conducting square loop of\[\begin{tabular}{|l|l|l|} \hline \multicolumn{3}{|c|}{\(\mathbf{\otimes} \mathbf{\otimes} \mathbf{\otimes} \mathbf{\otimes} \mathbf{\otimes} \mathbf{\otimes} \mathbf{\otimes} \mathbf{\otimes}\)} \\ \hline ⊗ & ⊗ல & \(\otimes \otimes \otimes \otimes\) \\ \hline QO & & － 00 \\ \hline 808 & & ⊕ \(\otimes \otimes\) \\ \hline \(\otimes \otimes\) & & ✓ 86 \\ \hline ⊗৫日 & & 目日 \\ \hline \[\otimes \otimes \mathbb{C}\] & & ⊗७Q \\ \hline & \(\otimes \otimes \otimes \otimes \otimes \otimes \otimes \otimes \otimes \otimes \otimes\) & \\ \hline & & \\ \hline \end{tabular}\]side L and resistance R moves in its plane with a uniform velocity v perpendicular to one of its sides. A magnetic induction constant in time and space, pointing perpendicular and
into the plane of the loop exists everywhere. The current induced in the loop is