It follows from symmetry considerations that the initial circuit can be replaced by an equivalent one (Fig. 215). We replace the "inner"
triangle consisting of an infinite number of elements by a resistor of resistance RAB/2, where the resistance RAB is such that RAB = Rx and RAB = aρ. After simplification, the circuit becomes a system of series- and parallel-connected conductors. In order to find Rx , we write the equation
Solving this equation, we obtain