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Exercises · 4.4

Q.To what extent do the electronic configurations decide the stability of oxidation states in the first series of the transition elements? Illustrate your answer with examples.

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The stability of oxidation states in the first transition series is largely decided by the electronic configuration, specifically the ability to achieve half-filled or fully-filled dd-subshells, and the balance between ionization energy and hydration energy. The +2 state is generally stable for all elements, but the +3 state becomes less stable across the series, with exceptions like CrX3+\ce{Cr^{3+}} (d3d^3) and MnX2+\ce{Mn^{2+}} (d5d^5) being particularly stable due to exchange energy and symmetry.

The first transition series (Sc to Zn) shows a fascinating variety of oxidation states. The key to understanding their stability lies in the electronic configuration of the ions, but it is not the only factor. Let’s break this down.

1. The role of electronic configuration

The stability of an oxidation state is primarily determined by the energy required to remove electrons (ionization enthalpy) and the energy released when the ion is stabilized in a compound (e.g., hydration energy, lattice energy). However, the electronic configuration of the ion itself provides a powerful clue.

For transition metals, the most stable oxidation states are those that lead to:

  • A half-filled dd-subshell (d5d^5), which has maximum exchange energy and symmetry.
  • A fully-filled dd-subshell (d10d^{10}), which is particularly stable due to complete pairing.
  • An empty dd-subshell (d0d^0), which is stable due to the absence of any dd-electron repulsion.

These configurations are not just arbitrary; they arise from the fact that electrons in half-filled or fully-filled subshells have lower energy because of exchange energy (Hund’s rule) and reduced electron-electron repulsion.

2. The +2 oxidation state: the baseline

For all elements in the first transition series, the +2 oxidation state is common. This is because the first two electrons removed are from the 4s orbital (which is filled before the 3d, but after removal, the 3d electrons remain). The +2 state corresponds to the configuration 3dn3d^n (where nn is the number of dd-electrons left after removing two 4s electrons).

  • Example: FeX2+\ce{Fe^{2+}} has configuration 3d63d^6, CoX2+\ce{Co^{2+}} has 3d73d^7, etc.
  • The +2 state is stable for all, but its relative stability varies. For instance, MnX2+\ce{Mn^{2+}} (d5d^5) is exceptionally stable because of the half-filled dd-subshell. Similarly, ZnX2+\ce{Zn^{2+}} (d10d^{10}) is very stable due to the fully-filled dd-subshell.
Watch out

A common mistake is to think that the +2 state is always the most stable. While it is common, it is not always the most stable for every element. For example, ScX2+\ce{Sc^{2+}} is not stable because ScX3+\ce{Sc^{3+}} (d0d^0) is much more stable.

3. The +3 oxidation state: a tale of two halves

The +3 state becomes less stable as we move across the series from left to right. This is because removing a third electron (from the 3d subshell) requires more energy, and the stabilization from the resulting configuration may or may not compensate.

  • Early elements (Sc to Cr): The +3 state is stable. For example:
    • ScX3+\ce{Sc^{3+}} (d0d^0) is very stable.
    • TiX3+\ce{Ti^{3+}} (d1d^1) is stable.
    • VX3+\ce{V^{3+}} (d2d^2) is stable.
    • CrX3+\ce{Cr^{3+}} (d3d^3) is particularly stable because the d3d^3 configuration has a half-filled t2gt_{2g} set in an octahedral field, giving extra crystal field stabilization energy (CFSE).
  • Middle elements (Mn to Fe): The +3 state is less stable. For example:
    • MnX3+\ce{Mn^{3+}} (d4d^4) is unstable and disproportionates into MnX2+\ce{Mn^{2+}} (d5d^5) and MnX4+\ce{Mn^{4+}} (d3d^3). The d4d^4 configuration is prone to Jahn-Teller distortion and is less stable than the d5d^5 of MnX2+\ce{Mn^{2+}}.
    • FeX3+\ce{Fe^{3+}} (d5d^5) is actually quite stable because of the half-filled dd-subshell. In fact, FeX3+\ce{Fe^{3+}} is more stable than FeX2+\ce{Fe^{2+}} in some environments (e.g., in acidic solution, FeX3+\ce{Fe^{3+}} is stable, but FeX2+\ce{Fe^{2+}} is easily oxidized).
  • Later elements (Co to Zn): The +3 state becomes increasingly unstable. For example:
    • CoX3+\ce{Co^{3+}} (d6d^6) is a strong oxidizing agent and is not stable in water (it oxidizes water to oxygen). However, in complexes like [Co(NHX3)X6]X3+\ce{[Co(NH3)6]^{3+}}, it is stabilized by strong field ligands.
    • NiX3+\ce{Ni^{3+}} (d7d^7) is very rare and unstable.
    • CuX3+\ce{Cu^{3+}} (d8d^8) is extremely rare.
    • ZnX3+\ce{Zn^{3+}} does not exist.

4. Higher oxidation states: the role of oxygen

Higher oxidation states (like +4, +5, +6, +7) are possible only when the metal is bonded to highly electronegative elements like oxygen or fluorine. This is because these ligands can stabilize the high positive charge through strong covalent bonding (e.g., in oxoanions).

  • Examples:
    • CrX6+\ce{Cr^{6+}} in CrOX4X2−\ce{CrO4^{2-}} (chromate) and CrX2OX7X2−\ce{Cr2O7^{2-}} (dichromate) is stable, but CrX6+\ce{Cr^{6+}} as a simple ion does not exist. The d0d^0 configuration of CrX6+\ce{Cr^{6+}} is stable.
    • MnX7+\ce{Mn^{7+}} in MnOX4X−\ce{MnO4^-} (permanganate) is stable, again with d0d^0 configuration.
    • FeX6+\ce{Fe^{6+}} in FeOX4X2−\ce{FeO4^{2-}} (ferrate) is known but is a strong oxidizing agent and less stable.
Tip

A useful shortcut: For a given element, the most stable oxidation state is often the one that gives a d0d^0, d5d^5, or d10d^{10} configuration. For example, Cr\ce{Cr} is most stable as CrX3+\ce{Cr^{3+}} (d3d^3) and CrX6+\ce{Cr^{6+}} (d0d^0), while Mn\ce{Mn} is most stable as MnX2+\ce{Mn^{2+}} (d5d^5) and MnX7+\ce{Mn^{7+}} (d0d^0).

5. The trend across the series

Let’s summarize the stability of common oxidation states for the first transition series:

ElementCommon oxidation statesMost stable state(s)Reason
Sc+3+3d0d^0 configuration

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