Quick Recap — Transition & Inner-transition Elements

  • Transition (d-block) elements have partially filled dd-orbitals; general config (n1)d110ns12(n-1)d^{1-10}\,ns^{1-2}; groups 3-12; first series Sc-Zn.
  • Characteristics: variable oxidation states, coloured ions (d-d transitions), paramagnetism (μ=n(n+2)\mu=\sqrt{n(n+2)} BM), catalytic activity, alloy and interstitial-compound formation, high melting points.
  • Lanthanoids (period 6, 4f) and actinoids (period 7, 5f) are inner-transition; common state +3+3; lanthanoid contraction makes Zr \approx Hf.
  • Key oxidisers: KMnO4KMnO_4 (Mn +7+7, purple), K2Cr2O7K_2Cr_2O_7 (Cr +6+6, orange).

Beyond-NCERT JEE Formulae

Use this as a JEE formula sheet for the d- and f-block. The chapter is mostly descriptive, so the ONE genuine calculation is the spin-only magnetic moment; everything else is a systematic trend. Each entry says WHEN to use it, and a [JEE Tip] flags the classic exam trap.

1. Spin-only Magnetic Moment

  • Master relation: μ=n(n+2)\mu=\sqrt{n(n+2)} BM, where nn is the number of UNPAIRED electrons. Use it whenever a question gives an ion (or its dxd^x count) and wants the magnetic moment, or gives a measured moment and wants nn.
  • Ready-reckoner: n=11.73n=1\to1.73, n=22.83n=2\to2.83, n=33.87n=3\to3.87, n=44.90n=4\to4.90, n=55.92n=5\to5.92 BM.
  • Back-calculation: square the moment, then solve n(n+2)=μ2n(n+2)=\mu^2. A measured 4.904.90 gives n(n+2)=24n(n+2)=24, so n=4n=4; a measured 3.873.87 gives 1515, so n=3n=3.
  • [JEE Tip] It is a SQUARE ROOT: for d5d^5, μ=35=5.92\mu=\sqrt{35}=5.92, never 3535. And count nn from the ION, not the atom (strip the 4s4s electrons first, see below).

2. Unpaired Electrons from the Ion Configuration

  • Golden rule of ionisation: the nsns electrons leave BEFORE the (n1)d(n-1)d. Build the ion by writing the neutral atom, removing both 4s4s electrons first, then taking any extra charge from 3d3d. Example: Fe is [Ar]3d64s2[Ar]3d^6 4s^2, so Fe2+ is 3d63d^6 and Fe3+ is 3d53d^5.
  • Unpaired count vs dxd^x (high-spin): d0d^0 0, d1d^1 1, d2d^2 2, d3d^3 3, d4d^4 4, d5d^5 5, d6d^6 4, d7d^7 3, d8d^8 2, d9d^9 1, d10d^{10} 0. The count climbs to a d5d^5 peak, then falls symmetrically.
  • Config exceptions (atoms): Cr is [Ar]3d54s1[Ar]3d^5 4s^1 and Cu is [Ar]3d104s1[Ar]3d^{10} 4s^1 (extra stability of half- and fully-filled dd). So a neutral Cr atom has 6 unpaired electrons, and Cu2+ is 3d93d^9 (1 unpaired), never 3d103d^{10}.
  • [JEE Tip] The commonest slip is using the atom's 3d64s23d^6 4s^2 for Fe2+; the ion is 3d63d^6 (4 unpaired). A transition-metal ION never keeps its 4s4s electrons.

3. Systematic Trends (with reasoning)

  • Variable oxidation states: (n1)d(n-1)d and nsns lie close in energy, so d-electrons count as valence electrons too; successive states then differ by one, e.g. Mn spans +2+2 to +7+7.
  • Highest OS peaks at Mn: the maximum oxidation state equals the total 3d+4s3d+4s electrons usable in bonding. It climbs from Sc (+3)(+3) up to Mn (+7)(+7), then FALLS (Fe tops out at +6+6) because the rising nuclear charge grips the d-electrons. So Mn shows the series' highest OS, +7+7 in KMnO4.
  • Lanthanoid contraction: the steady size fall across Ce to Lu, because the diffuse 4f4f electrons shield poorly and the effective nuclear charge rises. Consequences: (i) Zr and Hf have almost equal radii, (ii) the basic strength of Ln(OH)3 falls from La to Lu, (iii) the near-equal sizes make the lanthanoids hard to separate.
  • Colour needs a d-d transition: a partly filled dd-subshell is essential, so d0d^0 (Sc3+, Ti4+) and d10d^{10} (Zn2+, Cu+) ions are COLOURLESS, while d1d^1 to d9d^9 ions are coloured. An intense colour on a d0d^0 ion such as MnO4- (purple) comes from ligand-to-metal charge transfer, not a d-d jump.
  • [JEE Tip] "Colourless" and "diamagnetic" coincide only for d0d^0 and d10d^{10}; a half-filled d5d^5 ion (Mn2+) is faintly coloured and strongly paramagnetic, so do not call it colourless.

4. Electrode Potentials, Disproportionation and Observed Moments

  • E(M2+/M)E^\circ(M^{2+}/M) trend: generally NEGATIVE across the 3d series (the metals are reducing); copper alone is positive at +0.34+0.34 V, because its large ΔsubH+ΔiH\Delta_{sub}H+\Delta_iH is not repaid by the hydration enthalpy.
  • Irregularities: the extra-stable half-filled d5d^5 (Mn2+) and filled d10d^{10} (Zn2+) give unusually negative E(M2+/M)E^\circ(M^{2+}/M); for the M3+/M2+M^{3+}/M^{2+} couple, Cr2+ is a strong reductant (it forms the stable d3d^3 ion Cr3+) whereas Co3+ is a strong oxidant.
  • Disproportionation: 3MnO42+4H+2MnO4+MnO2+2H2O3MnO_4^{2-}+4H^+\to 2MnO_4^-+MnO_2+2H_2O (green manganate to purple permanganate plus brown MnO2); and 2Cu+Cu2++Cu2Cu^+\to Cu^{2+}+Cu in aqueous solution.
  • Spin-only vs observed: the formula ignores orbital motion, so ions with an unquenched orbital contribution (Co2+, Ni2+) show observed moments a little ABOVE the spin-only value; JEE writes "spin-only" when it wants the formula answer.
  • [JEE Tip] Only copper has a positive E(M2+/M)E^\circ(M^{2+}/M) in the 3d series; do not generalise it, since the rest are negative.

Solved Examples — Beyond-NCERT Formulae

Example 1 - Spin-only moment of Fe2+. Find the spin-only magnetic moment of the iron(II) ion.

  • Fe is [Ar]3d64s2[Ar]3d^6 4s^2; strip the 4s24s^2 pair first, so Fe2+ is 3d63d^6.
  • High-spin d6d^6 is t2g4eg2t_{2g}^4 e_g^2: one orbital is doubly filled and four are singly filled, so n=4n=4.
  • μ=4(4+2)=24=4.90\mu=\sqrt{4(4+2)}=\sqrt{24}=4.90 BM.

Example 2 - Spin-only moment of Mn2+. Find the spin-only moment of the manganese(II) ion.

  • Mn is [Ar]3d54s2[Ar]3d^5 4s^2; remove the 4s24s^2 pair, so Mn2+ is 3d53d^5.
  • Half-filled d5d^5 has every d-orbital singly occupied, so n=5n=5, the maximum for the 3d series.
  • μ=5(5+2)=35=5.92\mu=\sqrt{5(5+2)}=\sqrt{35}=5.92 BM. Fe3+ (also 3d53d^5) gives the same 5.92 BM.

Example 3 - Unpaired electrons from a measured moment. A first-series ion has spin-only μ=2.83\mu=2.83 BM. Find the number of unpaired electrons and name a possible ion.

  • Square the moment: n(n+2)=μ2=(2.83)28n(n+2)=\mu^2=(2.83)^2\approx 8.
  • Solve n2+2n8=0n^2+2n-8=0, i.e. (n+4)(n2)=0(n+4)(n-2)=0, giving n=2n=2.
  • A d8d^8 ion fits, e.g. Ni2+ (3d83d^8). Trap: reading 2.83 as 3 unpaired; n=3n=3 would give 3.873.87, not 2.83.

Example 4 - Order ions by magnetic moment. Arrange Ti3+, Ni2+, Cr3+ and Mn2+ in increasing spin-only moment.

  • Ion configs: Ti3+ is 3d13d^1, Cr3+ is 3d33d^3, Mn2+ is 3d53d^5, Ni2+ is 3d83d^8.
  • Unpaired electrons: Ti3+ 1, Ni2+ 2, Cr3+ 3, Mn2+ 5.
  • More unpaired electrons means a larger μ\mu, so the order is Ti3+ (1.73) < Ni2+ (2.83) < Cr3+ (3.87) < Mn2+ (5.92) BM.

Example 5 - Coloured vs colourless ions. Which of Sc3+, Ti3+, Cu2+, Zn2+ and Cu+ are colourless in dilute aqueous solution?

  • Colour needs a partly filled d-subshell for a d-d transition.
  • Sc3+ is 3d03d^0, Zn2+ is 3d103d^{10} and Cu+ is 3d103d^{10}: no d-d transition, so all three are COLOURLESS.
  • Ti3+ (3d13d^1, violet) and Cu2+ (3d93d^9, blue) have partly filled d-subshells, so they are COLOURED.
  • Colourless count =3=3.

Example 6 - Highest number of unpaired electrons. Among Fe2+, Fe3+, Co2+ and Ni2+, which ion has the most unpaired electrons?

  • Configs: Fe2+ is 3d63d^6 (4), Fe3+ is 3d53d^5 (5), Co2+ is 3d73d^7 (3), Ni2+ is 3d83d^8 (2).
  • The half-filled d5d^5 of Fe3+ wins with n=5n=5, so Fe3+ has the most (μ=35=5.92\mu=\sqrt{35}=5.92 BM).
  • Note Fe3+ beats Fe2+ despite having FEWER d-electrons, because d5d^5 maximises the unpaired spins.

Example 7 - The copper anomaly. Find the spin-only moment of Cu2+.

  • Cu is anomalous: [Ar]3d104s1[Ar]3d^{10} 4s^1, not 3d94s23d^9 4s^2.
  • Remove the 4s14s^1 electron (Cu+ is 3d103d^{10}), then one 3d3d electron, so Cu2+ is 3d93d^9.
  • Nine electrons in five d-orbitals leave one unpaired, n=1n=1, so μ=1(1+2)=3=1.73\mu=\sqrt{1(1+2)}=\sqrt{3}=1.73 BM.

Example 8 - The chromium anomaly (neutral atom). How many unpaired electrons, and what spin-only moment, does a neutral Cr atom have?

  • Cr adopts the extra-stable half-filled ground state [Ar]3d54s1[Ar]3d^5 4s^1, not 3d44s23d^4 4s^2.
  • All five 3d3d orbitals are singly filled (5) and the lone 4s4s electron adds one more, so n=6n=6.
  • μ=6(6+2)=48=6.93\mu=\sqrt{6(6+2)}=\sqrt{48}=6.93 BM, higher than any first-series ION because both subshells contribute unpaired electrons.