To solve this question, we need to understand and use the concepts of resistors connected in series and parallel. Let's break the problem down step-by-step:
- When resistances are connected in parallel, the reciprocal of the total (or equivalent) resistance \( R \) is the sum of the reciprocals of each individual resistance. If each resistance is \( r \) ohms and there are \( n \) such resistances in parallel, the formula is given by:
\(\frac{1}{R} = \frac{1}{r} + \frac{1}{r} + \ldots + \frac{1}{r}\)
(n times)
Resulting in:
\(\frac{1}{R} = \frac{n}{r}\)
- The equivalent resistance \( R \) for parallel configuration can be found by:
\(R = \frac{r}{n}\)
- Now, if these \( n \) resistances are connected in series, then the total resistance \( R_{\text{series}} \) is simply the sum of individual resistances. Hence, it is given by:
\(R_{\text{series}} = n \times r\)
- We derived that \( r = n \times R \) from the equivalent resistance of the parallel connection:
\(R = \frac{r}{n} \Rightarrow r = n \times R\)
- Substituting \( r = n \times R \) back into the equation for series resistance:
\(R_{\text{series}} = n \times (n \times R) = n^2 \times R\)
- Therefore, the total resistance when the resistors are connected in series is:
\(n^2 R\)
Conclusion: When the resistances are connected in series, the equivalent resistance is \( n^2 R \). Thus, the correct answer is:
n^2 R