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 sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
A constant voltage of 50 V is maintained between the points A and B of the circuit shown in the figure. The current through the branch CD of the circuit is :