In the network shown, each resistance is equal to R. The equivalent
resistance between diagonally opposite corners is:

R
$\frac{R}{3}$
$\frac{2 R}{3}$
$\frac{4 R}{3}$

\frac{R}{3}

\frac{4 R}{3}

\frac{2 R}{3}

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In the network shown, each resistance is equal to R. The equivalent
resistance between diagonally opposite corners is:

R
$\frac{R}{3}$
$\frac{2 R}{3}$
$\frac{4 R}{3}$