The problem begins with a wire of total resistance \( R \) divided into 8 equal segments. The resistance of each segment is calculated as:
\[ R_{\text{piece}} = \frac{R}{8} \]
Subsequently, four of these segments are connected in parallel. The equivalent resistance \( R_{\text{parallel}} \) for these parallel resistors is determined by:
\[ \frac{1}{R_{\text{parallel}}} = \frac{1}{R_{\text{piece}}} + \frac{1}{R_{\text{piece}}} + \frac{1}{R_{\text{piece}}} + \frac{1}{R_{\text{piece}}} = 4 \times \frac{1}{R_{\text{piece}}} \]
This simplifies to:
\[ R_{\text{parallel}} = \frac{R_{\text{piece}}}{4} = \frac{R/8}{4} = \frac{R}{32} \]
Two such parallel combinations are formed, each yielding a resistance of \( \frac{R}{32} \).
These two equivalent resistances are then connected in series. The total resistance \( R_{\text{total}} \) for series connections is the sum of individual resistances:
\[ R_{\text{total}} = R_{\text{parallel}} + R_{\text{parallel}} = \frac{R}{32} + \frac{R}{32} = \frac{2R}{32} = \frac{R}{16} = \frac{R}{4} \]
Consequently, the net effective resistance of the entire combination is \( \frac{R}{4} \).