When a uniform wire of resistance \( r \) is cut into \( n \) equal parts, the resistance of each part will be \( \frac{r}{n} \). This is because resistance is directly proportional to the length of the wire, and cutting it into \( n \) equal segments reduces the length of each segment to \( \frac{1}{n} \) of the original wire.
If you connect these \( n \) parts in series, the total resistance will be \( r_{\text{total}} = n \times \frac{r}{n} = r \), which is the same as the original resistance. However, if you connect them in parallel, the total resistance can be calculated using the formula:
\[
\frac{1}{R_{\text{total}}} = \frac{1}{\frac{r}{n}} + \frac{1}{\frac{r}{n}} + \ldots + \frac{1}{\frac{r}{n}} = \frac{n}{\frac{r}{n}} = \frac{n^2}{r}
\]
Thus,
\[
R_{\text{total}} = \frac{r}{n^2}
\]
So, the total resistance when the wire is cut into equal parts depends on whether the parts are connected in series or parallel.