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Q.[Fe(H2O)6]3+[Fe(H_2O)_6]^{3+} is strongly paramagnetic whereas [Fe(CN)6]3−[Fe(CN)_6]^{3-} is weakly paramagnetic. Explain.

Rajasthan RbseTextbookSubjective· 3mImportance★★★★★
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The difference in paramagnetic strength arises from the ligand field splitting: weak-field HX2O\ce{H2O} ligands leave FeX3+\ce{Fe^{3+}} with five unpaired electrons (high-spin, strong paramagnetism), while strong-field CNX−\ce{CN-} ligands cause pairing, leaving only one unpaired electron (low-spin, weak paramagnetism).

The key here is not just counting electrons — it’s understanding how the ligand environment reshapes the electron configuration of the central metal ion. Both complexes contain FeX3+\ce{Fe^{3+}}, which has a 3d53d^5 configuration. But the magnetic behaviour is dramatically different because the ligands control whether those five d-electrons remain unpaired or are forced into pairs.

Let’s walk through the reasoning step by step.

  1. Determine the oxidation state and d-electron count.

    In both complexes, iron is in the +3 oxidation state.

    Fe\ce{Fe} (atomic number 26) has the ground-state configuration [Ar] 3d64s2[\ce{Ar}]\,3d^6 4s^2.

    Losing three electrons (two from 4s and one from 3d) gives FeX3+\ce{Fe^{3+}}: 3d53d^5.

    So we have five electrons to place in the d-orbitals.

  2. Recall the effect of ligand field splitting in octahedral complexes.

    In an octahedral field, the five d-orbitals split into two sets:

    • Lower energy: t2gt_{2g} (three orbitals: dxy,dxz,dyzd_{xy}, d_{xz}, d_{yz})
    • Higher energy: ege_g (two orbitals: dx2−y2,dz2d_{x^2-y^2}, d_{z^2}) The energy gap between them is called Δo\Delta_o (or 10 Dq10\,Dq). The magnitude of Δo\Delta_o depends on the ligand: strong-field ligands (like CNX−\ce{CN-}) cause a large splitting; weak-field ligands (like HX2O\ce{H2O}) cause a small splitting.
  3. Apply Hund’s rule vs. pairing energy.

    For a d5d^5 configuration, there are two possible arrangements:

    • High-spin: electrons occupy all five orbitals singly before any pairing occurs. This requires Δo\Delta_o to be smaller than the pairing energy (PP).
    • Low-spin: electrons pair up in the t2gt_{2g} orbitals, leaving some orbitals empty. This happens when Δo>P\Delta_o > P.

    If Δo<P→high-spin;if Δo>P→low-spin\text{If } \Delta_o < P \rightarrow \text{high-spin}; \quad \text{if } \Delta_o > P \rightarrow \text{low-spin}

  4. Analyse [Fe(HX2O)X6]3+[\ce{Fe(H2O)6}]^{3+}.

    Water is a weak-field ligand. For FeX3+\ce{Fe^{3+}}, Δo\Delta_o for HX2O\ce{H2O} is about 13,700 cm−113{,}700\ \text{cm}^{-1}, while the pairing energy PP is roughly 17,600 cm−117{,}600\ \text{cm}^{-1}.

    Since Δo<P\Delta_o < P, the electrons avoid pairing.

    The five d-electrons occupy all five orbitals singly:

t2g3 eg2t_{2g}^3\ e_g^2

This gives five unpaired electrons.

Magnetic moment: μ=n(n+2)=5×7=35≈5.92 BM\mu = \sqrt{n(n+2)} = \sqrt{5 \times 7} = \sqrt{35} \approx 5.92\ \text{BM} — strongly paramagnetic.

  1. Analyse [Fe(CN)X6]3−[\ce{Fe(CN)6}]^{3-}. Cyanide is a strong-field ligand. For FeX3+\ce{Fe^{3+}}, Δo\Delta_o for CNX−\ce{CN-} is about 35,000 cm−135{,}000\ \text{cm}^{-1}, far above PP. Now Δo>P\Delta_o > P, so electrons pair up in the t2gt_{2g} orbitals before occupying ege_g. The configuration becomes:

t2g5 eg0t_{2g}^5\ e_g^0

This means four electrons are paired in two orbitals, and one electron remains unpaired in the third t2gt_{2g} orbital. …

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