Step 1: Apply the Irving--Williams series for M\(^{2+}\) (3d) complexes.
For high-spin octahedral divalent first-row transition metals, the thermodynamic stabilities of complexes (including chelates like en) follow:
\[
\text{Mn}^{2+}<\text{Fe}^{2+}<\text{Co}^{2+}<\text{Ni}^{2+}<\text{Cu}^{2+}>\text{Zn}^{2+}.
\]
Thus, among Co, Ni, Cu, and Fe, the \emph{least} stable chelate is for Fe\(^{2+}\).
Step 2: Rationalize using LFSE and additional stabilization.
The chelate effect favors \([M(en)_3]^{2+}\) for all M, but relative stabilities are governed by metal-dependent factors. Approximate octahedral LFSE (high spin) values:
\[
\begin{aligned}
\text{Fe}^{2+} (d^6\ \text{HS}) &: -0.4\,\Delta_o,
\text{Co}^{2+} (d^7\ \text{HS}) &: -0.8\,\Delta_o,
\text{Ni}^{2+} (d^8) &: -1.2\,\Delta_o,
\text{Cu}^{2+} (d^9) &: \text{JT stabilization (very strong)}.
\end{aligned}
\]
Smaller (less negative) LFSE for Fe\(^{2+}\) leads to a less stable octahedral complex than Co\(^{2+}\) and Ni\(^{2+}\). Cu\(^{2+}\) is exceptionally stabilized overall despite Jahn--Teller distortion, consistent with the Irving--Williams series.
Step 3: Conclusion.
Therefore, the formation of \([M(en)_3]^{2+}\) from \([M(H_2O)_6]^{2+}\) is \underline{least favored} when \(M=\text{Fe}\).