The d- and f- Block Elements

Iron nails, silver jewellery, the gold in a wedding ring, the vanadium pentoxide that manufactures sulphuric acid by the tonne, the manganese dioxide inside a torch battery, and the deep purple flash of a permanganate titration — the d-block sits at the practical heart of chemistry, and this chapter is the map of why. Groups 3 to 12 of the periodic table hold the transition metals, elements whose (n minus 1)d orbitals are being progressively filled while the outermost ns orbital stays almost static; tucked below the main table, the f-block lanthanoids and actinoids fill 4f and 5f orbitals instead. Together they explain some of the most useful, and most heavily tested, chemistry in the CBSE and JEE and NEET syllabus: why chromium's configuration is 3d5 4s1 and not the naively expected 3d4 4s2, why manganese alone among the 3d metals reaches the +7 state, why copper sulphate solutions are blue while zinc sulphate is colourless, and why zirconium and hafnium are so alike in size and behaviour that separating them industrially is notoriously difficult. This article walks through the whole unit in NCERT's own order: electronic configurations and physical trends of the 3d series, the logic of oxidation-state stability built from ionisation enthalpies and exchange energy, electrode potentials and why Cu2+ is stable in water while Cu+ disproportionates, magnetic moments and coloured ions, the manufacture and redox chemistry of potassium dichromate and potassium permanganate, and finally the lanthanoids and actinoids. Four trend derivations and four solved numericals connect every rule to a concrete calculation, because JEE and NEET test this chapter less as bare definitions and more as "which ion is coloured," "predict the stable oxidation state," and "balance this redox equation."

Key takeaways
  • d-block = groups 3-12, general outer configuration (n−1)d1−10ns1−2(n-1)d^{1-10}ns^{1-2}, arranged in four series: 3d (Sc to Zn), 4d (Y to Cd), 5d (La and Hf to Hg) and 6d (Ac and Rf to Cn); the f-block sits below as a separate panel, 4f lanthanoids (Ce to Lu) and 5f actinoids (Th to Lr).
  • Zn, Cd and Hg have a full d10 configuration in the atom and in their common ions, so by the modern IUPAC definition they are not called transition elements even though they physically sit in the d-block.
  • Cr (3d5 4s1) and Cu (3d10 4s1) break the naive filling order because half-filled and fully filled d subshells carry extra exchange-energy stability that a simple 3d4 4s2 or 3d9 4s2 picture misses.
  • Melting points, atomisation enthalpies and metallic bonding strength peak near the middle of the 3d series (roughly at Cr and V, and again at Fe-Co-Ni) with a sharp dip at manganese, because the number of unpaired d electrons available for interatomic bonding is what drives the strength of the metal-metal bond.
  • Oxidation states in the d-block differ from each other by one (not by two, as in the p-block); manganese shows the widest range of any 3d metal, from +2 to +7, and the highest oxidation state up to Mn tracks the sum of s and d electrons.
  • Electrode potentials and ion stability trace back to d0, d5 and d10 stability: Sc3+ (d0), Mn2+ and Fe3+ (both d5), and Zn2+ and Cu+ (d10) are all anomalously stable compared with their neighbours.
  • Partly filled d orbitals cause coloured, paramagnetic ions; the number of unpaired electrons n predicts the magnetic moment through the spin-only formula μ=n(n+2)\mu = \sqrt{n(n+2)} Bohr magneton, and d0 or d10 ions (Sc3+, Ti4+, Zn2+, Cu+) are colourless because no d-d transition is possible.
  • Potassium dichromate (orange, Cr2O7 2-) and potassium permanganate (purple, MnO4-) are the two must-know oxidising agents of the chapter, each manufactured from an ore (chromite, pyrolusite) and each reduced to a definite lower state (Cr3+, Mn2+) in acidic titrations.
  • Lanthanoid contraction — the steady shrinkage of ionic radius across the 4f-filling lanthanoids, caused by poor 4f shielding — makes Zr and Hf almost identical in size and chemistry; a sharper version, actinoid contraction, does the same across the 5f series.
  • Key idea: partly filled (n-1)d or 4f/5f orbitals give transition and inner-transition elements variable oxidation states differing by one, coloured paramagnetic ions governed by the spin-only formula, and exceptional stability at d0, d5 and d10 configurations that explains chromium's anomalous configuration, the oxidising power of dichromate and permanganate, and — through lanthanoid contraction — the near-twin chemistry of zirconium and hafnium.
The core insight

Partly filled d (transition, d-block) or f (inner-transition, f-block) orbitals give these elements variable oxidation states differing by one, paramagnetic coloured ions predicted by the spin-only formula μ=n(n+2)\mu = \sqrt{n(n+2)}, and special stability at d0, d5 and d10 (or f0, f7, f14) configurations that governs everything from chromium's anomalous 3d5 4s1 configuration to the oxidising power of dichromate and permanganate to the near-identical chemistry of zirconium and hafnium via lanthanoid contraction.

What this chapter covers

This article follows the chapter's own sequence: position and configuration (where the d- and f-blocks sit, the four transition series, the (n−1)d ns(n-1)d\,ns pattern and its Cr/Cu exceptions), then the general properties of the 3d series one at a time — physical properties and atomisation enthalpy, atomic/ionic radii, ionisation enthalpies, oxidation states, the M2+/M and M3+/M2+ electrode potentials, stability of higher oxidation states, and magnetic, colour, catalytic, interstitial and alloy behaviour. A dedicated section covers the chapter's two named compounds, potassium dichromate and potassium permanganate. The article then turns to the f-block — lanthanoids (contraction, oxidation states) and actinoids (radioactivity, a wider oxidation-state range, comparison with lanthanoids) — closing with the industrial applications that make this chapter genuinely load-bearing.

The core ideas

Position, series and electronic configuration

The d-block occupies the broad middle section of the periodic table, flanked by the s-block and the p-block. Moving across a period, electrons fill the (n−1)d(n-1)d orbitals — the penultimate shell — giving four rows: the 3d series (Sc to Zn, Z 21-30), the 4d series (Y to Cd, Z 39-48), the 5d series (La, then Hf to Hg, Z 57 and 72-80) and the 6d series (Ac, then Rf to Cn, Z 89 and 104-112). The f-block sits as a separate panel below: the 4f series, Ce to Lu, the lanthanoids, and the 5f series, Th to Lr, the actinoids. The general outer electronic configuration of the d-block is

(n−1)d1−10 ns1−2(n-1)d^{1-10}\,ns^{1-2}

where: nn is the principal quantum number of the outermost shell, (n−1)d(n-1)d holds one to ten electrons, and nsns normally holds one or two — except palladium, 4d105s04d^{10}5s^{0}. Chromium is 3d54s13d^{5}4s^{1}, not the naively expected 3d44s23d^{4}4s^{2}, and copper is 3d104s13d^{10}4s^{1}, not 3d94s23d^{9}4s^{2}; both trace to the extra stability of half-filled and fully filled d subshells, derived in full below. By the modern IUPAC definition, a transition element has an incompletely filled d subshell in the neutral atom or in a common ion — a sharper test than "sits in the d-block." Zinc, cadmium and mercury are d10d^{10} in the atom and stay d10d^{10} in their only common ion, +2+2, so none counts as a transition element despite sitting at the d-block's edge; scandium (3d14s23d^{1}4s^{2}) does count, because that one 3d electron is incomplete.

Figure
Schematic periodic table showing the s block, the p block, the d block split into its four transition series 3d 4d 5d and 6d, and the f block lanthanoid and actinoid panel placed below the main table
Where the d-block and f-block sit in the periodic table s-block, groups 1-2 d-block, groups 3 to 12 3d series: Sc to Zn, Z 21-30 4d series: Y to Cd, Z 39-48 5d series: La and Hf to Hg, Z 57, 72-80 6d series: Ac and Rf to Cn, Z 89, 104-112 p-block, groups 13-18 f-block, 4f lanthanoids: Ce to Lu, Z 58-71 f-block, 5f actinoids: Th to Lr, Z 90-103 La (Z 57) and Ac (Z 89) sit at the head of the 5d and 6d rows but are usually discussed with the f-block

General physical properties: metallic character, melting points and atomisation enthalpy

Nearly all transition elements show classic metallic behaviour — high tensile strength, ductility, malleability, thermal and electrical conductivity, metallic lustre — in hcp, bcc or ccp lattices (Zn, Cd, Hg and Mn are anomalous). Their melting and boiling points are high because the (n−1)d(n-1)d electrons join the nsns electrons in metallic bonding, giving more bonding electrons per atom than the neighbouring s- or p-block metals. Across a row, melting point and atomisation enthalpy rise toward a maximum near the middle and fall again, with a sharp dip at manganese. Metal-metal bond strength depends on the number of unpaired d electrons, so bonding peaks where unpairing is greatest and weakens as d orbitals pair up toward d10d^{10}; manganese's comparatively unreactive, half-filled 3d54s23d^{5}4s^{2} bonds less effectively than its neighbours. The 4d and 5d series also have systematically higher atomisation enthalpies than the corresponding 3d metals, which is why metal-metal bonding in compounds is far more common among the heavier transition metals.

Figure
Line graph of enthalpy of atomisation in kilojoules per mole across the 3d series from scandium to zinc, rising to a first peak near vanadium, dipping sharply at manganese, rising again to a second peak around nickel, then falling steeply at zinc
Enthalpy of atomisation across the 3d series 0 200 400 600 kJ/mol Sc Ti V Cr Mn Fe Co Ni Cu Zn dip at Mn — stable half filled 3d5 4s2, weaker bonding Zn falls sharply — no d electrons join metallic bonding

Atomic and ionic radii: the first sighting of lanthanoid contraction

Ionic radii of the same charge decrease steadily across a series, because each added electron enters an inner d orbital that shields the outer shell only imperfectly, so effective nuclear charge rises and pulls the shell in; atomic radii show the same trend but vary less than in the s- and p-blocks. Comparing series, atomic radii grow noticeably from the 3d row to the 4d row, but the 5d row is almost the same size as the 4d row rather than growing further — because fourteen 4f electrons fill between lanthanum and hafnium, and the resulting lanthanoid contraction (derived below) shrinks the 5d atoms enough to cancel the expected increase. Zirconium (160 pm) and hafnium (159 pm) end up almost identical in radius.

Ionisation enthalpies and the special stability of d0, d5 and d10

Ionisation enthalpy rises across each series left to right, driven by the same rising effective nuclear charge, but far more gently than across an s- or p-block period, because the added and removed electrons sit in different, only partially shielding subshells (3d3d versus 4s4s). The first ionisation enthalpy rises only slightly and somewhat irregularly; the second and third rise more steeply once 4s4s electrons are gone, but with sharp breaks exactly where a d5d^{5} configuration is created or destroyed — the second ionisation enthalpy of manganese and the third of iron are both unusually high because the ion formed (Mn2+\text{Mn}^{2+} or Fe3+\text{Fe}^{3+}) is the extra-stable 3d53d^{5}, and removing yet another electron sacrifices that stability. The mechanism, exchange energy among parallel-spin electrons in degenerate orbitals, is derived fully below, since it also governs oxidation-state and electrode-potential stability.

Oxidation states across the 3d series

One of the most distinctive features of transition metals is the sheer number of oxidation states a single element can show. Scandium is essentially locked into +3+3; manganese, near the middle, exhibits every state from +2+2 to +7+7; copper and zinc are largely restricted to low states because too many d electrons are left to accommodate a high one. Up to manganese, the maximum reasonably stable state equals the sum of ss and dd electrons — TiIV\text{Ti}^{IV} in TiO2\text{TiO}_2, VV\text{V}^{V} in VO2+\text{VO}_2^{+}, CrVI\text{Cr}^{VI} in CrO42−\text{CrO}_4^{2-}, MnVII\text{Mn}^{VII} in MnO4−\text{MnO}_4^{-} — after which stability drops abruptly, so Fe, Co, Ni, Cu and Zn are typically FeII,III\text{Fe}^{II,III}, CoII,III\text{Co}^{II,III}, NiII\text{Ni}^{II}, CuI,II\text{Cu}^{I,II} and ZnII\text{Zn}^{II}. d-block oxidation states differ from one another by one unit (VII,VIII,VIV,VV\text{V}^{II}, \text{V}^{III}, \text{V}^{IV}, \text{V}^{V}), not the two typical of the p-block's inert-pair effect. Down a group the trend also reverses: heavier p-block elements favour lower states, but heavier d-block elements favour higher ones — molybdenum(VI) and tungsten(VI) are markedly more stable than chromium(VI), which is exactly why acidified dichromate, wanting to drop from +6+6 to the stable +3+3, is a strong oxidant while MoO3\text{MoO}_3 and WO3\text{WO}_3 are not.

Standard electrode potentials: M2+/M and M3+/M2+

The E⊖(M2+/M)E^{\ominus}(\text{M}^{2+}/\text{M}) values become less negative from titanium to copper, tracking the rising sum of the first two ionisation enthalpies. Manganese and zinc sit more negative than the trend predicts because Mn2+\text{Mn}^{2+} (3d53d^5) and Zn2+\text{Zn}^{2+} (3d103d^{10}) are unusually stable, and nickel because of its very large hydration enthalpy. Copper is the outlier with a positive E⊖(Cu2+/Cu)=+0.34 VE^{\ominus}(\text{Cu}^{2+}/\text{Cu}) = +0.34\ \text{V}: it cannot displace hydrogen from dilute acids, because the energy to atomise and ionise solid copper is not fully repaid by its hydration enthalpy. The E⊖(M3+/M2+)E^{\ominus}(\text{M}^{3+}/\text{M}^{2+}) values tell a complementary story: low for scandium (Sc3+\text{Sc}^{3+}, noble-gas-like, so easy to form), high for manganese (Mn2+\text{Mn}^{2+}, d5d^5, resists further oxidation), low for iron (Fe3+\text{Fe}^{3+}, d5d^5, easy to form this time), and low for vanadium (stable half-filled t2gt_{2g} in V2+\text{V}^{2+}). These four values are a compact summary of how d0d^{0} and d5d^{5} stability governs which oxidation state a 3d metal prefers in solution.

Stability of higher oxidation states: the role of fluorine and oxygen

Only fluorine and oxygen reliably stabilise a metal's very highest oxidation states. Fluorine works through high lattice energy (CoF3\text{CoF}_3) or strong covalent bonds (VF5\text{VF}_5, CrF6\text{CrF}_6), but has limits — manganese's +7+7 state has no simple fluoride, only MnO3F\text{MnO}_3\text{F}. Oxygen is the stronger stabiliser because it can form multiple (π\pi) bonds to the metal, so covalent Mn2O7\text{Mn}_2\text{O}_7 exists though the highest manganese fluoride is only MnF4\text{MnF}_4. As oxidation number rises, oxides grow less ionic and more acidic: Sc2O3\text{Sc}_2\text{O}_3 is basic, V2O5\text{V}_2\text{O}_5 is amphoteric, CrO3\text{CrO}_3 gives H2CrO4\text{H}_2\text{CrO}_4/H2Cr2O7\text{H}_2\text{Cr}_2\text{O}_7, and Mn2O7\text{Mn}_2\text{O}_7 gives the strong acid HMnO4\text{HMnO}_4.

Magnetic properties and coloured ions

Unpaired electrons in partly filled d orbitals make most transition-metal ions paramagnetic; ions with none are diamagnetic. For first-row compounds the orbital contribution is effectively quenched, so the moment is predicted from the number of unpaired electrons alone using the spin-only formula:

μ=n(n+2) BM\mu = \sqrt{n(n+2)}\ \text{BM}

where: μ\mu is the magnetic moment in Bohr magneton (BM) and nn is the number of unpaired electrons. One unpaired electron gives μ≈1.73 BM\mu \approx 1.73\ \text{BM}; five (a d5d^{5} ion such as Mn2+\text{Mn}^{2+} or Fe3+\text{Fe}^{3+}) give μ≈5.92 BM\mu \approx 5.92\ \text{BM}, the largest first-row value. Measuring μ\mu experimentally is therefore a direct way to count unpaired electrons and pin down configuration and oxidation state. Colour follows a related mechanism: visible light excites an electron from a lower to a higher d orbital, and the colour seen is complementary to the frequency absorbed. This needs a partly filled d subshell, so d0d^{0} or d10d^{10} ions cannot show it and are colourless — Sc3+\text{Sc}^{3+}, Ti4+\text{Ti}^{4+}, Cu+\text{Cu}^{+} and Zn2+\text{Zn}^{2+} are all colourless, while V3+\text{V}^{3+} (green), Mn2+\text{Mn}^{2+} (pale pink), Fe3+\text{Fe}^{3+} (yellow) and Cu2+\text{Cu}^{2+} (blue) are coloured. The exact shade also depends on the ligand bound — the start of the ligand-field ideas developed fully in the coordination-compounds chapter that follows.

Complex formation, catalysis, interstitial compounds and alloys

Transition metals form unusually many complexes — [Fe(CN)6]3−[\text{Fe}(\text{CN})_6]^{3-}, [Cu(NH3)4]2+[\text{Cu}(\text{NH}_3)_4]^{2+}, [PtCl4]2−[\text{PtCl}_4]^{2-} — because their ions are small, highly charged, and have empty or partly filled d orbitals to accept ligand electron pairs. The same variable oxidation states make them excellent catalysts: V2O5\text{V}_2\text{O}_5 in the Contact Process, iron in the Haber process, nickel in hydrogenation. A clean example is Fe3+\text{Fe}^{3+} catalysing 2I−+S2O82−→I2+2SO42−2\text{I}^{-} + \text{S}_2\text{O}_8^{2-} \rightarrow \text{I}_2 + 2\text{SO}_4^{2-}: the direct reaction is slow (both reactants are negatively charged), but Fe3+\text{Fe}^{3+} oxidises I−\text{I}^{-} to I2\text{I}_2 while becoming Fe2+\text{Fe}^{2+}, which S2O82−\text{S}_2\text{O}_8^{2-} then reoxidises — a two-step relay avoiding the slow like-charge collision.

Interstitial compounds form when small atoms (H, C, N) sit trapped inside a metal lattice, giving non-stoichiometric formulas (TiC\text{TiC}, Fe3H\text{Fe}_3\text{H}, VH0.56\text{VH}_{0.56}) with no normal oxidation state; they are very hard, have higher melting points than the pure metal, stay metallically conductive, and are chemically inert. Alloys form readily because transition-metal radii are usually within fifteen percent of each other — steels (Cr, V, W, Mo, Mn), brass (Cu-Zn) and bronze (Cu-Sn) are the industrially dominant examples.

Potassium dichromate and potassium permanganate

These are the two named compounds NCERT singles out, each built from an ore, isolated as a solid oxidant, and used in acidified titrations. Potassium dichromate, K2Cr2O7\text{K}_2\text{Cr}_2\text{O}_7, comes from chromite ore, FeCr2O4\text{FeCr}_2\text{O}_4, by oxidative fusion with sodium carbonate in air to sodium chromate, acidified to sodium dichromate, then converted to the less soluble potassium salt with KCl (full sequence in the fourth derivation below). Chromate (tetrahedral CrO42−\text{CrO}_4^{2-}) and dichromate (two corner-shared tetrahedra, Cr-O-Cr\text{Cr-O-Cr} angle 126∘126^{\circ}) interconvert with pH — acid gives orange dichromate, alkali reverses it. In acid, dichromate is a strong oxidant, Cr2O72−+14H++6e−→2Cr3++7H2O\text{Cr}_2\text{O}_7^{2-} + 14\text{H}^{+} + 6e^{-} \rightarrow 2\text{Cr}^{3+} + 7\text{H}_2\text{O} (E⊖=+1.33 VE^{\ominus} = +1.33\ \text{V}), oxidising iodide, tin(II), sulphide and iron(II).

Potassium permanganate, KMnO4\text{KMnO}_4, comes from pyrolusite, MnO2\text{MnO}_2, fused with alkali and an oxidant (KNO3_3 or air) to dark green potassium manganate, K2MnO4\text{K}_2\text{MnO}_4, then oxidised — commercially by electrolysis, or by disproportionation in acid (3MnO42−+4H+→2MnO4−+MnO2+2H2O3\text{MnO}_4^{2-} + 4\text{H}^{+} \rightarrow 2\text{MnO}_4^{-} + \text{MnO}_2 + 2\text{H}_2\text{O}) — to purple permanganate. Its reduction depends sharply on pH: to manganate in strong alkali (E⊖=+0.56 VE^{\ominus} = +0.56\ \text{V}), to brown MnO2\text{MnO}_2 in neutral/faint alkali (E⊖=+1.69 VE^{\ominus} = +1.69\ \text{V}), and to nearly colourless Mn2+\text{Mn}^{2+} in acid (MnO4−+8H++5e−→Mn2++4H2O\text{MnO}_4^{-} + 8\text{H}^{+} + 5e^{-} \rightarrow \text{Mn}^{2+} + 4\text{H}_2\text{O}, E⊖=+1.52 VE^{\ominus} = +1.52\ \text{V}) — the reaction used in acidified titrations against iron(II), oxalate and hydrogen sulphide.

The lanthanoids: contraction and oxidation states

Lanthanum and the fourteen elements after it, cerium to lutetium (symbol Ln\text{Ln}), form the lanthanoid series. All share a common 6s26s^{2} outer configuration, filling 4f4f with increasing irregularity, but every Ln3+\text{Ln}^{3+} ion is a clean 4fn4f^{n}, because lanthanoids overwhelmingly favour +3+3. Ionic radii shrink steadily from La3+\text{La}^{3+} to Lu3+\text{Lu}^{3+}, the lanthanoid contraction, from imperfect shielding of one 4f4f electron by another (derived fully below). A few lanthanoids show +2+2 or +4+4, and every exception follows the same empty/half-filled/fully-filled stability logic as the 3d series: Ce4+\text{Ce}^{4+} (4f04f^{0}) is a slow-acting oxidant (E⊖=+1.74 VE^{\ominus} = +1.74\ \text{V}); Eu2+\text{Eu}^{2+} (4f74f^{7}) and Yb2+\text{Yb}^{2+} (4f144f^{14}) are reducing agents that revert to Ln3+\text{Ln}^{3+}; Tb4+\text{Tb}^{4+} (4f74f^{7}) is an oxidant. Trivalent ions other than La3+\text{La}^{3+} (f0f^0) and Lu3+\text{Lu}^{3+} (f14f^{14}) are paramagnetic and often coloured, from narrow ff-ff transitions. Early lanthanoids behave somewhat like calcium, later ones like aluminium; all liberate hydrogen from dilute acids, burn in halogens, and form basic Ln2O3\text{Ln}_2\text{O}_3 and Ln(OH)3\text{Ln}(\text{OH})_3. Mischmetall (about 95% Ln, 5% Fe) goes into lighter flints and Mg alloys; mixed Ln oxides are petroleum-cracking catalysts and screen phosphors.

The actinoids: wider oxidation states and comparison with the lanthanoids

The actinoid series, thorium to lawrencium (Z 90-103), is entirely radioactive, with the heaviest members short-lived and studied only in nanogram quantities. All share 7s27s^{2} with irregular 5f5f/6d6d occupancy; because 5f5f orbitals are less buried than 4f4f, they bond far more readily, giving actinoids a richer chemistry. +3+3 is the general state, but early actinoids reach unusually high maxima — Th +4+4, Pa +5+5, U +6+6, Np +7+7 — before narrowing back to +3+3 for later, more lanthanoid-like members. Actinoid contraction parallels lanthanoid contraction but is sharper, since 5f5f electrons shield each other even less effectively. Both series contract steadily in ionic radius, favour +3+3, and are silvery, reactive metals with basic hydroxides; but actinoids show a far wider oxidation-state range (especially early on), lower and less regular ionisation enthalpies, and — being radioactive — greater difficulty of study. Lanthanoid contraction remains the more chemically important effect, since it directly governs the well-studied near-identical chemistry of zirconium/hafnium and niobium/tantalum.

Applications in industry

Iron and steel remain the dominant construction materials, alloyed with Cr, Mn, V, W and Mo for hardness and corrosion resistance. TiO2\text{TiO}_2 is a workhorse pigment; MnO2\text{MnO}_2 powers dry-cell batteries; Zn and Ni-Cd power rechargeable ones. V2O5\text{V}_2\text{O}_5 catalyses the Contact Process, TiCl4\text{TiCl}_4/Al(CH3)3\text{Al}(\text{CH}_3)_3 forms the Ziegler catalyst for polythene, iron catalyses the Haber process, nickel catalyses hydrogenation, and PdCl2\text{PdCl}_2 catalyses the Wacker oxidation of ethyne to ethanal. AgBr\text{AgBr} underlies photography, and silver, gold and copper remain the historic "coinage metals."

Derivation AWhy chromium and copper break the naive filling order

The naive Aufbau expectation for the twenty-fourth and twenty-ninth elements is a smooth 3d44s23d^{4}4s^{2} for chromium and 3d94s23d^{9}4s^{2} for copper. Experiment instead finds 3d54s13d^{5}4s^{1} and 3d104s13d^{10}4s^{1}. The goal here is to show, using exchange energy among parallel-spin electrons, why moving one electron from 4s4s into 3d3d actually lowers the total energy in exactly these two cases.

Step 1. Recall exchange energy. When several electrons occupy a set of degenerate orbitals such as the five 3d orbitals, quantum mechanics rewards every pair of same-spin electrons in different orbitals with a small stabilisation. Hund's rule — maximum multiplicity — is the practical consequence: the state with the most such parallel-spin pairs is lowest in energy.

Step 2. Count pairs for chromium. In 3d44s23d^{4}4s^{2}, four parallel 3d electrons give (42)=6\binom{4}{2} = 6 exchange pairs. In 3d54s13d^{5}4s^{1}, five parallel 3d electrons give (52)=10\binom{5}{2} = 10 pairs — four more — while the 4s electron contributes nothing either way.

Step 3. Weigh the trade-off. Promoting one 4s4s electron into 3d3d costs a small orbital-energy penalty, since the two orbitals are close in energy, but buys four extra exchange pairs at essentially no added repulsion. For Cr and Cu this payoff exceeds the cost; for neighbours like V or Ni it does not, since their configuration would not reach a half-filled or fully filled subshell. The same logic applies to copper's 3d103d^{10}, and the identical anomaly reappears at silver and gold one and two rows down.

Go deeper · Derivation B · 1 minThe d5 break in ionisation enthalpy and oxidation-state stability across the 3d series
Derivation BThe d5 break in ionisation enthalpy and oxidation-state stability across the 3d series

Successive ionisation enthalpies of the 3d metals do not increase smoothly; instead there are sharp breaks exactly where a d5d^{5} configuration is created or destroyed. The goal here is to derive why removing an electron from a d5d^{5} ion is unusually hard, why removing one to reach d5d^{5} is unusually easy, and to connect that directly to which oxidation states of Cr, Mn and Fe are actually found stable.

Step 1. Count exchange pairs at d5d^{5}. Five electrons in five d orbitals, all parallel by Hund's rule, give (52)=10\binom{5}{2} = 10 exchange pairs — the maximum possible for a d subshell, since no other electron count can put every electron in its own orbital with parallel spin.

Step 2. Compare a d6d^{6} ion (one doubly occupied orbital, four single) with d5d^{5}: removing the paired electron relieves Coulomb repulsion and maximises exchange pairs at once, so d6→d5d^{6}\to d^{5} is easy. Removing a further electron from the already-maximised d5d^{5}, to d4d^{4}, destroys that 10-pair arrangement and is unusually costly.

Step 3. Apply this to real ions and read off the electrode-potential pattern. Fe2+\text{Fe}^{2+} (3d63d^{6}) loses an electron to Fe3+\text{Fe}^{3+} (3d53d^{5}) unusually easily — the third ionisation enthalpy of iron is lower than a smooth trend predicts, and E⊖(Fe3+/Fe2+)E^{\ominus}(\text{Fe}^{3+}/\text{Fe}^{2+}) is comparatively low — so Fe3+\text{Fe}^{3+} is iron's everyday stable state. Mn2+\text{Mn}^{2+} (3d53d^{5}) is already at the maximum, so oxidising it to Mn3+\text{Mn}^{3+} (3d43d^{4}) is unusually costly and E⊖(Mn3+/Mn2+)E^{\ominus}(\text{Mn}^{3+}/\text{Mn}^{2+}) is comparatively high, making Mn2+\text{Mn}^{2+} far more stable than Mn3+\text{Mn}^{3+}. The same logic explains why Cr2+\text{Cr}^{2+} (d4d^{4}) is strongly reducing, eagerly reaching the more stable Cr3+\text{Cr}^{3+} (d3d^{3}, half-filled t2gt_{2g}), while Mn3+\text{Mn}^{3+} (d4d^{4}) is strongly oxidising, eagerly falling into extra-stable Mn2+\text{Mn}^{2+} (d5d^{5}).

Go deeper · Derivation C · 1 minLanthanoid contraction and why zirconium and hafnium are chemical twins
Derivation CLanthanoid contraction and why zirconium and hafnium are chemical twins

The goal here is to trace how a purely atomic-scale effect — poor shielding of one 4f electron by another — produces a macroscopic, industrially important consequence: zirconium (4d series, Z 40) and hafnium (5d series, Z 72) have almost identical radii even though a full row of fourteen extra protons separates them.

Step 1. Start from the shielding rule. An inner electron partially shields outer electrons from the nucleus, and how effective that shielding is depends on orbital shape: more diffuse, higher-angular-momentum orbitals shield less well. The 4f orbitals are the most diffuse, least effective shielders of any commonly filled subshell — even less effective than 3d.

Step 2. Apply this across the fourteen lanthanoids: from lanthanum (Z 57) to lutetium (Z 71), one electron fills 4f and one proton is added at each step, and since 4f electrons shield poorly, each new proton is felt almost fully by the outer shell, pulling it in — a small, relentless radius decrease at every step.

Step 3. Compare this with the size increase normally expected from adding a whole new shell (3d to 4d). Between lanthanum and hafnium, the cumulative contraction from those fourteen 4f elements is large enough to almost cancel that expected increase, which is why zirconium (160 pm) and hafnium (159 pm) end up essentially equal, while titanium (147 pm) is clearly smaller than both.

Step 4. Because Zr and Hf (and similarly Nb/Ta, Mo/W) are so alike in size, they are alike in almost every other property, occur together in the same ores, and are notoriously difficult to separate chemically — the single most examined consequence of lanthanoid contraction.

Go deeper · Derivation D · 1 minMechanism of manufacture: chromite ore to potassium dichromate
Derivation DMechanism of manufacture: chromite ore to potassium dichromate

The goal here is to walk through the sequence that converts insoluble chromite ore into pure, crystalline potassium dichromate, tracking chromium's oxidation state and the solubility logic at each stage.

Step 1. Oxidative alkali fusion. Chromite, FeCr2O4\text{FeCr}_2\text{O}_4 (Cr already +3+3), is fused with sodium carbonate in air; oxygen oxidises chromium to +6+6 and iron to +3+3: 4FeCr2O4+8Na2CO3+7O2→8Na2CrO4+2Fe2O3+8CO24\text{FeCr}_2\text{O}_4 + 8\text{Na}_2\text{CO}_3 + 7\text{O}_2 \rightarrow 8\text{Na}_2\text{CrO}_4 + 2\text{Fe}_2\text{O}_3 + 8\text{CO}_2. Insoluble Fe2O3\text{Fe}_2\text{O}_3 is filtered off; yellow sodium chromate passes into solution — the step that separates chromium from iron.

Step 2. Acidification to sodium dichromate: 2Na2CrO4+2H+→Na2Cr2O7+2Na++H2O2\text{Na}_2\text{CrO}_4 + 2\text{H}^{+} \rightarrow \text{Na}_2\text{Cr}_2\text{O}_7 + 2\text{Na}^{+} + \text{H}_2\text{O}. Chromium's oxidation state stays +6+6 throughout; only the anion's structure changes, single tetrahedral CrO42−\text{CrO}_4^{2-} to corner-shared Cr2O72−\text{Cr}_2\text{O}_7^{2-}, as acid pushes the equilibrium right.

Step 3. Cation exchange to the potassium salt: Na2Cr2O7+2KCl→K2Cr2O7+2NaCl\text{Na}_2\text{Cr}_2\text{O}_7 + 2\text{KCl} \rightarrow \text{K}_2\text{Cr}_2\text{O}_7 + 2\text{NaCl}. Potassium dichromate is far less soluble than sodium chloride under these conditions, so it crystallises out selectively — a solubility-driven metathesis, not a redox step.

Step 4. The chromate-dichromate equilibrium stays pH-reversible throughout: alkali converts dichromate back to chromate, Cr2O72−+2OH−→2CrO42−+H2O\text{Cr}_2\text{O}_7^{2-} + 2\text{OH}^{-} \rightarrow 2\text{CrO}_4^{2-} + \text{H}_2\text{O}, and re-acidifying reverses it. This is why the standard oxidising half-reaction, Cr2O72−+14H++6e−→2Cr3++7H2O\text{Cr}_2\text{O}_7^{2-} + 14\text{H}^{+} + 6e^{-} \rightarrow 2\text{Cr}^{3+} + 7\text{H}_2\text{O} (E⊖=+1.33 VE^{\ominus} = +1.33\ \text{V}), and every dichromate titration, is always run in acid.

Worked examples

Board level - spin-only magnetic moment of a divalent 3d ion (extends NCERT Example 4.8)

An element has atomic number 25. Find the electronic configuration and the spin-only magnetic moment of its divalent ion in aqueous solution, and state whether the ion is coloured.

Step 1. Identify the element and its divalent ion. Atomic number 25 is manganese, ground-state configuration [Ar]3d54s2[\text{Ar}]3d^{5}4s^{2}. Forming Mn2+\text{Mn}^{2+} removes the two 4s4s electrons first (as it always does for d-block ions), leaving the configuration 3d53d^{5}.

Step 2. Count unpaired electrons using Hund's rule. Five electrons distributed across five degenerate 3d3d orbitals occupy each orbital singly with parallel spin, so n=5n = 5 unpaired electrons.

Step 3. Apply the spin-only formula: μ=n(n+2)=5×7=35=5.92 BM\mu = \sqrt{n(n+2)} = \sqrt{5 \times 7} = \sqrt{35} = 5.92\ \text{BM}.

Step 4. Decide on colour. Since 3d53d^{5} is neither d0d^{0} nor d10d^{10}, a dd-dd transition is possible, so Mn2+\text{Mn}^{2+} is coloured (observed as pale pink in aqueous solution). Answer: Mn2+\text{Mn}^{2+} has configuration 3d53d^{5}, magnetic moment 5.92 BM5.92\ \text{BM}, and is coloured (pale pink).

Board level - stoichiometry of potassium dichromate oxidising iron(II) (extends NCERT Exercise 4.15)

What volume of 0.100 M0.100\ \text{M} acidified potassium dichromate solution is required to completely oxidise the Fe2+\text{Fe}^{2+} present in 25.0 mL25.0\ \text{mL} of 0.600 M0.600\ \text{M} iron(II) sulphate solution?

Step 1. Write the balanced ionic equation. Dichromate's half-reaction is Cr2O72−+14H++6e−→2Cr3++7H2O\text{Cr}_2\text{O}_7^{2-} + 14\text{H}^{+} + 6e^{-} \rightarrow 2\text{Cr}^{3+} + 7\text{H}_2\text{O}, and iron(II)'s is Fe2+→Fe3++e−\text{Fe}^{2+} \rightarrow \text{Fe}^{3+} + e^{-}. Multiplying the iron half-reaction by 6 and adding gives Cr2O72−+14H++6Fe2+→2Cr3++6Fe3++7H2O\text{Cr}_2\text{O}_7^{2-} + 14\text{H}^{+} + 6\text{Fe}^{2+} \rightarrow 2\text{Cr}^{3+} + 6\text{Fe}^{3+} + 7\text{H}_2\text{O}, so the mole ratio is 1 mole of dichromate to 6 moles of Fe2+\text{Fe}^{2+}.

Step 2. Compute moles of Fe2+\text{Fe}^{2+} available: n(Fe2+)=0.600 mol/L×0.0250 L=0.0150 moln(\text{Fe}^{2+}) = 0.600\ \text{mol/L} \times 0.0250\ \text{L} = 0.0150\ \text{mol}.

Step 3. Convert to moles of dichromate required using the 1:6 ratio: n(Cr2O72−)=0.0150/6=2.50×10−3 moln(\text{Cr}_2\text{O}_7^{2-}) = 0.0150/6 = 2.50\times10^{-3}\ \text{mol}.

Step 4. Convert to volume: V=n/C=2.50×10−3 mol/0.100 mol/L=0.0250 LV = n/C = 2.50\times10^{-3}\ \text{mol} / 0.100\ \text{mol/L} = 0.0250\ \text{L}. Answer: 25.0 mL25.0\ \text{mL} of the 0.100 M0.100\ \text{M} dichromate solution is required.

Competitive level (JEE / NEET) - predicting colour and relative stability across a set of ions (extends NCERT Exercise 4.18)

Among Ti4+\text{Ti}^{4+}, V3+\text{V}^{3+}, Cu+\text{Cu}^{+}, Sc3+\text{Sc}^{3+}, Mn2+\text{Mn}^{2+}, Fe3+\text{Fe}^{3+} and Co2+\text{Co}^{2+}, identify which are coloured in aqueous solution, and state which single ion is most resistant to further oxidation.

Step 1. Write each ion's d-electron count. Ti4+\text{Ti}^{4+}: [Ar]3d0[\text{Ar}]3d^{0}. V3+\text{V}^{3+}: [Ar]3d2[\text{Ar}]3d^{2}. Cu+\text{Cu}^{+}: [Ar]3d10[\text{Ar}]3d^{10}. Sc3+\text{Sc}^{3+}: [Ar]3d0[\text{Ar}]3d^{0}. Mn2+\text{Mn}^{2+}: [Ar]3d5[\text{Ar}]3d^{5}. Fe3+\text{Fe}^{3+}: [Ar]3d5[\text{Ar}]3d^{5}. Co2+\text{Co}^{2+}: [Ar]3d7[\text{Ar}]3d^{7}.

Step 2. Apply the d0d^{0}/d10d^{10} colourless rule. Ti4+\text{Ti}^{4+} and Sc3+\text{Sc}^{3+} (d0d^{0}) and Cu+\text{Cu}^{+} (d10d^{10}) have no dd-dd transition available and are colourless; V3+\text{V}^{3+} (d2d^{2}, green), Mn2+\text{Mn}^{2+} (d5d^{5}, pale pink), Fe3+\text{Fe}^{3+} (d5d^{5}, pale yellow/violet depending on ligand) and Co2+\text{Co}^{2+} (d7d^{7}, pink) are all coloured.

Step 3. Rank stability against further oxidation using the d5d^{5} exchange-energy argument developed in the second derivation. Among these seven ions, Mn2+\text{Mn}^{2+} is the one whose configuration is already the maximally exchange-stabilised 3d53d^{5}, so oxidising it further to Mn3+\text{Mn}^{3+} (3d43d^{4}) is energetically unfavourable — consistent with the very high, oxidising E⊖(Mn3+/Mn2+)=+1.5 VE^{\ominus}(\text{Mn}^{3+}/\text{Mn}^{2+}) = +1.5\ \text{V} reported for this couple.

Step 4. State the answer clearly. Answer: Ti4+\text{Ti}^{4+}, Cu+\text{Cu}^{+} and Sc3+\text{Sc}^{3+} are colourless (d0d^0 or d10d^{10}); V3+\text{V}^{3+}, Mn2+\text{Mn}^{2+}, Fe3+\text{Fe}^{3+} and Co2+\text{Co}^{2+} are coloured; and Mn2+\text{Mn}^{2+} is the most resistant to further oxidation because it already holds the extra-stable half-filled 3d53d^{5} configuration. Timing note: under ninety seconds once the d0d^0/d5d^5/d10d^{10} checklist is automatic. Write only each species' outer dnd^{n} count and scan for n=0n = 0 or n=10n = 10 — everything else is coloured by default. Do not waste time recalling the exact shade unless asked.

Competitive level (JEE / NEET) - permanganate titration of oxalic acid, volume back-calculation

A 10.0 mL10.0\ \text{mL} sample of an oxalic acid solution requires 16.0 mL16.0\ \text{mL} of 0.0200 M0.0200\ \text{M} acidified KMnO4\text{KMnO}_4 for complete oxidation to CO2\text{CO}_2, at 333 K333\ \text{K}. Find the molarity of the oxalic acid solution.

Step 1. Write the balanced ionic equation. Permanganate in acid: MnO4−+8H++5e−→Mn2++4H2O\text{MnO}_4^{-} + 8\text{H}^{+} + 5e^{-} \rightarrow \text{Mn}^{2+} + 4\text{H}_2\text{O}. Oxalate: C2O42−→2CO2+2e−\text{C}_2\text{O}_4^{2-} \rightarrow 2\text{CO}_2 + 2e^{-}. Equalising electrons (multiply the first by 2, the second by 5) and adding gives 2MnO4−+5C2O42−+16H+→2Mn2++10CO2+8H2O2\text{MnO}_4^{-} + 5\text{C}_2\text{O}_4^{2-} + 16\text{H}^{+} \rightarrow 2\text{Mn}^{2+} + 10\text{CO}_2 + 8\text{H}_2\text{O}, a mole ratio of 22 permanganate to 55 oxalate.

Step 2. Compute moles of KMnO4\text{KMnO}_4 used: n(MnO4−)=0.0200 mol/L×0.0160 L=3.20×10−4 moln(\text{MnO}_4^{-}) = 0.0200\ \text{mol/L} \times 0.0160\ \text{L} = 3.20\times10^{-4}\ \text{mol}.

Step 3. Convert to moles of oxalic acid using the 2:52:5 ratio: n(C2O42−)=3.20×10−4×(5/2)=8.00×10−4 moln(\text{C}_2\text{O}_4^{2-}) = 3.20\times10^{-4} \times (5/2) = 8.00\times10^{-4}\ \text{mol}.

Step 4. Convert to molarity in the original 10.0 mL10.0\ \text{mL} sample: C=n/V=8.00×10−4 mol/0.0100 L=0.0800 mol/LC = n/V = 8.00\times10^{-4}\ \text{mol} / 0.0100\ \text{L} = 0.0800\ \text{mol/L}. Answer: the oxalic acid solution is 0.0800 M0.0800\ \text{M}. Timing note: about a minute and a half. This titration's mole ratio is not the intuitive 1:11{:}1 — always derive it from electron balance. It is self-indicating (permanganate's own colour vanishes at the endpoint) and run hot, since the reaction is slow at room temperature until autocatalysed by the Mn2+\text{Mn}^{2+} produced.

Common traps

The single most common slip is treating "d-block element" and "transition element" as synonyms. Zinc, cadmium and mercury sit in the d-block by position but fail the IUPAC test, since their d subshell is completely full (d10d^{10}) in both atom and common ion — a distinction examiners test directly. A second error is deleting ion electrons from the wrong shell. nsns electrons are always removed before (n−1)d(n-1)d electrons on ionisation, regardless of filling order in the neutral atom — so Fe\text{Fe} gives Fe2+\text{Fe}^{2+} as 3d63d^{6}, not 3d44s23d^{4}4s^{2}. Students often assume oxidation states differ by two, carrying the p-block's inert-pair habit across by reflex; d-block states differ by one. Relatedly, many wrongly say heavier d-block elements favour lower oxidation states "by the inert-pair effect" — the d-block trend runs the opposite way (Mo(VI)\text{Mo}(\text{VI}), W(VI)\text{W}(\text{VI}) more stable than Cr(VI)\text{Cr}(\text{VI})). A further slip is quoting a metal's highest oxidation state from its chloride rather than its oxide or fluoride — only fluorine and oxygen are small/electronegative (or, for oxygen, multiply-bonding) enough to reach the very highest states. Finally, a common arithmetic error is assuming permanganate or dichromate reacts mole-for-mole with a reducing agent. The ratio must be derived from electron balance (5 electrons per MnO4−\text{MnO}_4^{-} in acid, 6 per Cr2O72−\text{Cr}_2\text{O}_7^{2-}), and it changes if the medium changes, since permanganate's product itself changes from Mn2+\text{Mn}^{2+} to MnO2\text{MnO}_2 to MnO42−\text{MnO}_4^{2-}.

You should be able to…

  • State the modern IUPAC definition of a transition element and correctly exclude Zn, Cd and Hg using it.
  • Write the general outer electronic configuration of a d-block atom and its ion, applying the "nsns before (n−1)d(n-1)d" removal rule.
  • Explain, using exchange energy, why chromium and copper adopt 3d54s13d^{5}4s^{1} and 3d104s13d^{10}4s^{1} rather than the naively expected configurations.
  • Describe how melting point, atomisation enthalpy, atomic radius and ionic radius vary across the 3d series and explain the anomalies at manganese and zinc.
  • Predict which oxidation states of a given 3d metal are most stable, using the d0d^{0}/d5d^{5}/d10d^{10} special-stability rule and the "differ by one" spacing.
  • Use the spin-only formula to calculate the magnetic moment of an ion from its number of unpaired electrons, and predict whether an ion is coloured from its dnd^{n} configuration.
  • Describe the manufacture of potassium dichromate from chromite ore and potassium permanganate from pyrolusite, and write balanced ionic equations for their oxidising reactions in acid.
  • Define lanthanoid contraction, explain its cause, and connect it to the near-identical chemistry of zirconium and hafnium.
  • Compare lanthanoids and actinoids on electronic configuration, oxidation states, ionic-radius contraction and chemical reactivity.
  • Balance redox equations involving dichromate and permanganate and use them to solve titration and stoichiometry numericals.

Ask the tutor: Want to work through a full periodic-trends comparison table for the 3d, 4d and 5d series, or practice more dichromate/permanganate titration numericals until the electron-balancing becomes automatic?

Why are zinc, cadmium and mercury placed in the d-block but not called transition elements?

Position in the periodic table and the technical definition of "transition element" are two different things. Zinc, cadmium and mercury sit in group 12 at the right edge of the d-block, but by the neutral ground-state atom their dd subshell is already completely full (3d104s23d^{10}4s^{2} for zinc, and analogously for Cd and Hg), and their only common ion, +2+2, is also d10d^{10}. Since IUPAC requires an incomplete d subshell in the atom or a common ion, these three fail the test despite belonging geographically to the d-block. Their chemistry is still taught alongside the transition metals, since they are the natural end members of the 3d, 4d and 5d rows.

Why does chromium have the configuration 3d5 4s1 instead of the expected 3d4 4s2?

Because a half-filled d subshell carries extra "exchange energy" stability that a naive electron-filling diagram does not show. When five electrons occupy five different d orbitals with parallel spins, quantum mechanics rewards every pair of same-spin electrons in different orbitals with a small energy bonus; going from 3d43d^4 (four such pairs) to 3d53d^5 (ten such pairs) gains far more exchange stabilisation than the small energy cost of promoting one electron from the very close-lying 4s4s orbital into 3d3d. The same logic, taken to its fully-filled conclusion, explains why copper is 3d104s13d^{10}4s^1 rather than 3d94s23d^9 4s^2, and why silver and gold show the identical pattern one and two rows down.

Why is Mn2+ so much more stable than Mn3+, while Fe3+ is more stable than Fe2+?

Both cases trace back to the special stability of the half-filled 3d53d^{5} configuration. Mn2+\text{Mn}^{2+} already has the exchange-stabilised 3d53d^5 arrangement, so oxidising it further to Mn3+\text{Mn}^{3+} (3d43d^4) means giving up that stability, which costs energy and makes Mn3+\text{Mn}^{3+} a strong oxidising agent that readily falls back to Mn2+\text{Mn}^{2+}. Iron sits one element further along: Fe2+\text{Fe}^{2+} is 3d63d^{6}, one electron past the stable point, so oxidising it to Fe3+\text{Fe}^{3+} (3d53d^5) actually gains exchange stability rather than losing it, which is why Fe3+\text{Fe}^{3+} is comparatively easy to form and is the more stable everyday oxidation state of iron in most of its common compounds.

What exactly is lanthanoid contraction, and why does it matter beyond the lanthanoids themselves?

Lanthanoid contraction is the steady, cumulative shrinkage of atomic and ionic radius across the fourteen lanthanoid elements, caused by the poor ability of 4f electrons to shield each other from the increasing nuclear charge. On its own this would just be a curiosity about a row of unfamiliar metals, but its real importance is downstream: the fourteen lanthanoids sit between lanthanum and hafnium in the periodic table, so their cumulative contraction almost exactly cancels the size increase that adding hafnium's extra electron shell would otherwise produce. The result is that zirconium and hafnium (and, to a lesser extent, niobium and tantalum) end up nearly identical in radius and therefore in chemistry, which is why they occur together in nature and are genuinely difficult to separate industrially.

Why do transition-metal ions form coloured solutions while ions like Zn2+ and Sc3+ are colourless?

Colour in transition-metal ions comes from an electron absorbing a photon of visible light and jumping from one partly filled d orbital to another, higher-energy one; the colour you see is the complementary colour of whatever wavelength got absorbed. This kind of transition is only possible if the d subshell is partly filled, so there is at least one vacant d orbital for an electron to jump into and at least one occupied d orbital for it to jump from. Zn2+\text{Zn}^{2+} (3d103d^{10}) has no vacant d orbital at all, and Sc3+\text{Sc}^{3+} (3d03d^{0}) has no d electron to promote in the first place, so neither ion can absorb visible light this way and both appear colourless.

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