
- A$I_{AC}$ =$\sqrt 2 $$I_{EF}$
- B$\sqrt 2 $$I_{AC}=I_{EF}$
- C$I_{AO}=3I_{EF}$
- ✓$I_{AC}=I_{EF}$

${I_z} = {I_x} + {I_y}\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,or,\,\,{I_z} = 2{I_y}$
$\begin{array}{l}
\left( {\,{I_x} = {I_y}\,by\,symmetry\,of\,the\,figure} \right)\\
\therefore \,{I_{EF}} = \frac{{{I_z}}}{2}\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,...\left( i \right)
\end{array}$
Again, by the same theorem
$\begin{array}{l}
{I_z} = {I_{AC}} + {I_{BD}} = 2{I_{AC}}\\
\left( {\therefore \,{I_{AC}} = {I_{BD}}\,by\,symmetry\,of\,the\,figure} \right)\\
\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\therefore \,{I_{AC}} = \frac{{{I_z}}}{2}\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,...\left( {ii} \right)
\end{array}$
From $(i)$ and $(ii)$, we get ${I_{EF}} = {I_{AC}}$
Generate a complete, print-ready paper with questions like this in minutes — across 16+ boards, with answer keys.
$\phi=2 t^3+4 t^2+2 t+5 \;W b$
The magnitude of induced $emf$ in the coil at $t=5\; s$ is $..........\,V$.



$HC \equiv CH\mathop {\xrightarrow{{{\text{1% HgS}}{{\text{O}}_{\text{4}}}}}}\limits_{20\% {H_2}S{O_4}} A\xrightarrow{{C{H_3}MgX}}B\xrightarrow{{[O]}}$