To solve this problem, we need to understand the configuration of resistors in the hexagon. The hexagon is formed by six sides, each with a resistance of \(r \, \Omega\), and all vertices of the hexagon are connected to the center with the same resistance, \(r \, \Omega\).
- We label the corners of the hexagon as \(A, B, C, D, E,\) and \(F\). Let the center of the hexagon be point \(O\).
- We're asked for the equivalent resistance between two opposite corners, say \(A\) and \(D\), when current enters at \(A\) and leaves at \(D\).
- The hexagon and its connections create a symmetric network. The symmetry helps in simplifying the problem by making intelligent guesses about equal potential points.
- Since the arrangement is symmetric, the potential at \(B\) and \(F\) must be the same. Similarly, \(C\) and \(E\) will share the same potential.
- The resistors between opposite pairs can be combined using series-parallel rules:
- Resistors \(AB\), \(BO\), and \(OF\) are in series.
- This series combination is parallel to \(BF\).
- By symmetry and applying similar logic to other parts of the hexagon, we evaluate the net resistance between \(A\) and \(D\).
- Applying Kirchhoff's laws or the star-delta transformation method can efficiently solve such circuits.
After solving through methods such as delta-star transformations, it turns out that the resistance between any two opposite corners, considering incoming and outgoing currents, results in an equivalent resistance of:
\(\dfrac{4}{5} r\).
Thus, the correct option is \(\dfrac{4}{5} r\).