d and f Block Elements: Edge Cases and Subtle Traps (5)

medium 3 min read

Question

Calculate the spin-only magnetic moment of Fe3+\text{Fe}^{3+} and Mn2+\text{Mn}^{2+} ions in their high-spin state. Comment on which is more paramagnetic.

Solution — Step by Step

Fe\text{Fe} (Z = 26): [Ar]3d64s2[Ar] 3d^6 4s^2. Fe3+\text{Fe}^{3+}: lose 4s24s^2 first, then one 3d3d. Configuration: [Ar]3d5[Ar] 3d^5. Five unpaired electrons in high-spin.

Mn\text{Mn} (Z = 25): [Ar]3d54s2[Ar] 3d^5 4s^2. Mn2+\text{Mn}^{2+}: lose 4s24s^2. Configuration: [Ar]3d5[Ar] 3d^5. Five unpaired electrons (half-filled 3d3d).

μspin=n(n+2) BM (Bohr Magnetons)\mu_{spin} = \sqrt{n(n+2)} \text{ BM (Bohr Magnetons)}

where nn is the number of unpaired electrons.

μ=5(5+2)=355.92 BM\mu = \sqrt{5(5+2)} = \sqrt{35} \approx 5.92 \text{ BM}

Both ions have μ5.92\mu \approx 5.92 BM — equally paramagnetic in spin-only terms. They both have d5d^5 configuration with 55 unpaired electrons.

Final answer: μ(Fe3+)=μ(Mn2+)5.92\mu(\text{Fe}^{3+}) = \mu(\text{Mn}^{2+}) \approx 5.92 BM.

Why This Works

The spin-only formula assumes orbital angular momentum is “quenched” — true for first-row transition metals in most coordination environments, where the crystal field splits orbitals such that orbital motion is suppressed.

Both Fe3+\text{Fe}^{3+} and Mn2+\text{Mn}^{2+} are isoelectronic (both have 2424 electrons) and have the half-filled d5d^5 configuration, giving identical magnetic moments in spin-only treatment.

μspin=n(n+2) BM\mu_{spin} = \sqrt{n(n+2)} \text{ BM}

nnμ\mu (BM)
11.73
22.83
33.87
44.90
55.92

Alternative Method

Direct memorisation: for d5d^5 high-spin, μ=5.92\mu = 5.92 BM. JEE often gives multiple ions; for each, just read off the dnd^n count and look up the value.

For NEET, memorise that Mn2+,Fe3+\text{Mn}^{2+}, \text{Fe}^{3+}, and any d5d^5 high-spin ion have the same spin-only magnetic moment (355.92\sqrt{35} \approx 5.92 BM). This appeared in NEET 2022 directly.

Common Mistake

The five classic d-block traps:

  1. Counting all dd electrons as unpaired: only the truly unpaired ones contribute. For low-spin d6d^6 (like [Fe(CN)6]4[\text{Fe(CN)}_6]^{4-}), all six pair up → n=0μ=0n = 0 \to \mu = 0 BM (diamagnetic).

  2. Removing 3d3d electrons before 4s4s: when forming cations, 4s4s electrons are removed first, then 3d3d. So FeFe2+\text{Fe} \to \text{Fe}^{2+} loses 4s24s^2, giving 3d63d^6, not 3d44s23d^4 4s^2.

  3. Mixing high-spin and low-spin: depends on the ligand strength. Strong-field ligands (CN^-, CO) cause low-spin; weak-field (H2_2O, F^-) cause high-spin. Default to high-spin if not specified.

  4. Forgetting that lanthanides have orbital contribution: for f-block, the spin-only formula doesn’t work — must use μ=gJ(J+1)\mu = g\sqrt{J(J+1)} with JJ the total angular momentum.

  5. Confusing the units (BM vs J/T): 1 Bohr Magneton = 9.274×10249.274 \times 10^{-24} J/T. JEE/NEET answers are conventionally in BM.

The fix: write the configuration carefully, identify nn, apply the formula. For lanthanides, switch to the full Landé formula.

Want to master this topic?

Read the complete guide with more examples and exam tips.

Go to full topic guide →

Try These Next