Step 1: Read the layout from the figure
Electrode order along a line is \(\mathrm{C1}\), \(\mathrm{C2}\), \(\mathrm{P1}\), \(\mathrm{P2}\) with \emph{equal spacing} \(a\) between adjacent electrodes.
Step 2: Recognize dipoles
- \(\mathrm{C1}\)–\(\mathrm{C2}\) form the \emph{current dipole} of length \(a\).
- \(\mathrm{P1}\)–\(\mathrm{P2}\) form the \emph{potential dipole} of length \(a\).
- The gap between the two dipoles is the spacing between \(\mathrm{C2}\) and \(\mathrm{P1}\), which is also \(a\). Hence the centers of the two dipoles are separated by \(2a\) (from \(x=\tfrac{a}{2}\) to \(x=\tfrac{5a}{2}\)).
Step 3: Match with the dipole–dipole definition
In a Dipole–Dipole array, two equal-length dipoles (current and potential) are laid out colinearly, and the center-to-center separation is \(n a\) where \(n\) is an integer (\(n\ge 1\)).
Here each dipole length \(= a\) and center-to-center separation \(= 2a\) \(\Rightarrow\) \(n=2\). This precisely matches a dipole–dipole configuration with \(n=2\).
Step 4: Rule out other arrays
- Wenner: Order is typically \(\mathrm{C1}\)–\(\mathrm{P1}\)–\(\mathrm{P2}\)–\(\mathrm{C2}\) with equal spacing; the potential pair sits \emph{between} the current electrodes. Not the case here.
- Schlumberger: Current electrodes far apart, potential electrodes close together near the center; spacings are unequal. Not the case here.
- Pole–Pole: Uses one current and one potential electrode with remote returns at infinity. Not applicable.
\[
\boxed{\text{Therefore, the array is Dipole–Dipole (with } n=2\text{).}}
\]