To solve this problem, we start with a wire of total resistance \( R \) that is cut into 8 equal pieces. Each piece will thus have a resistance of:
\[ R_{\text{piece}} = \frac{R}{8} \]
Next, four of these pieces are connected in parallel to form one equivalent resistance. The formula for calculating the equivalent resistance \( R_{\text{parallel}} \) of resistors in parallel (with equal resistance) is:
\[ \frac{1}{R_{\text{parallel}}} = \frac{1}{R_{\text{piece}}} + \frac{1}{R_{\text{piece}}} + \frac{1}{R_{\text{piece}}} + \frac{1}{R_{\text{piece}}} = 4 \times \frac{1}{R_{\text{piece}}} \]
Simplifying, we find:
\[ R_{\text{parallel}} = \frac{R_{\text{piece}}}{4} = \frac{R/8}{4} = \frac{R}{32} \]
Since we create two equivalent resistances using the same method (four pieces in parallel each), both will have the same resistance \( \frac{R}{32} \).
These two are then added in series, and the total resistance \( R_{\text{total}} \) for resistors in series is simply the sum:
\[ R_{\text{total}} = R_{\text{parallel}} + R_{\text{parallel}} = \frac{R}{32} + \frac{R}{32} = \frac{2R}{32} = \frac{R}{16} = \frac{R}{4} \]
Therefore, the net effective resistance of the combination is \( \frac{R}{4} \).
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) is :