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Resistance n, each of r ohm, when connec...

Resistance `n`, each of `r ohm`, when connected in parallel give an equivalent resistance of `R ohm`. If these resistances were connected series, the combination would have a resistance in ohm, equal to

A

`n^(2) R`

B

`R // n^(2)`

C

`R // n`

D

nR

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The correct Answer is:
To solve the problem, we need to find the equivalent resistance when `n` resistors, each of resistance `r ohm`, are connected in series, given that their equivalent resistance when connected in parallel is `R ohm`. ### Step-by-Step Solution: 1. **Understanding Parallel Resistance**: The formula for the equivalent resistance \( R \) of \( n \) resistors each of resistance \( r \) connected in parallel is given by: \[ \frac{1}{R} = \frac{1}{r} + \frac{1}{r} + \ldots + \frac{1}{r} \quad (n \text{ times}) \] This can be simplified to: \[ \frac{1}{R} = \frac{n}{r} \] Therefore, we can express \( R \) as: \[ R = \frac{r}{n} \] 2. **Finding Individual Resistance**: From the equation above, we can rearrange it to find \( r \): \[ r = nR \] 3. **Understanding Series Resistance**: When the same \( n \) resistors are connected in series, the equivalent resistance \( R_{eq} \) is simply the sum of all individual resistances: \[ R_{eq} = r + r + \ldots + r \quad (n \text{ times}) = n \times r \] 4. **Substituting the Value of \( r \)**: Now, substituting the value of \( r \) from step 2 into the series resistance formula: \[ R_{eq} = n \times (nR) = n^2 R \] 5. **Final Result**: Thus, the equivalent resistance when the resistors are connected in series is: \[ R_{eq} = n^2 R \] ### Conclusion: The equivalent resistance when the resistors are connected in series is \( n^2 R \).

To solve the problem, we need to find the equivalent resistance when `n` resistors, each of resistance `r ohm`, are connected in series, given that their equivalent resistance when connected in parallel is `R ohm`. ### Step-by-Step Solution: 1. **Understanding Parallel Resistance**: The formula for the equivalent resistance \( R \) of \( n \) resistors each of resistance \( r \) connected in parallel is given by: \[ \frac{1}{R} = \frac{1}{r} + \frac{1}{r} + \ldots + \frac{1}{r} \quad (n \text{ times}) ...
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