Electronic Configurations of d-Block Elements
Iron rusts, copper turns a statue green, and a purple potassium permanganate crystal can tint an entire beaker of water — transition metals are chemically loud in a way that sodium or calcium never are. The reason traces back to one place: how their electrons are arranged. In the d-block, the last electron to be added goes into an inner (n−1)d orbital even while the outer ns orbital is already occupied, and that inward filling is what gives these elements their variable oxidation states, colour and catalytic power. This article stays inside the opening section of Class 12's "d- and f-Block Elements" chapter: the general electronic configuration of the d-block, the first (3d) transition series from scandium to zinc, the two famous exceptions chromium and copper, and the rule for building the configuration of a transition-metal ion. Two fully worked configurations anchor the method, and the traps section flags the mistakes examiners see most often.
d-block atoms fill electrons into (n−1)d orbitals after the ns orbital is occupied, so their general configuration is , with chromium and copper breaking the naive Aufbau count for extra half-filled or fully-filled stability, and ions forming by losing ns electrons before any (n−1)d electron.
The core idea
Where the d-block sits. The d-block occupies Groups 3 to 12, wedged between the s-block and the p-block. An atom belongs to the d-block when its highest-energy electron, added last, enters an (n−1)d subshell rather than the outer ns or np subshell — even though the ns orbital was filled first, in order of increasing energy.
The general valence configuration for any d-block atom is written as
where: is the outermost shell's principal quantum number, the exponent on ranges from 1 to 10 depending on how many d electrons the element carries, and the exponent on is usually 2 (occasionally 1 or, for the d-block ions, 0). For the first transition series this becomes the concrete, exam-ready form built on the argon core:
running from scandium (Z = 21) to zinc (Z = 30).
The two Aufbau exceptions. A half-filled () or fully-filled () d-subshell carries extra stability because it maximises exchange energy — the stabilising effect that arises when several electrons of parallel spin, all in orbitals of identical energy, can swap positions. Two elements in the 3d series adopt this more-stable arrangement instead of the naive Aufbau prediction:
- Chromium (Z = 24): expected [Ar], actual [Ar].
- Copper (Z = 29): expected [Ar], actual [Ar].
The figure below lines up the full 3d series so the two anomalies are visible against the regular pattern.
Forming ions. When a transition-metal atom loses electrons to become a cation, the ns electrons are removed first, not the (n−1)d electrons — even though d filled after s during atom-building. Once an atom is ionised, the (n−1)d orbital drops below ns in energy, so the s electrons are the ones lost. For example, Fe ([Ar]) loses both 4s electrons to give Fe = [Ar], and loses one further d electron to give Fe = [Ar]. Zinc ([Ar]) and its ion Zn (= [Ar]) always carry a completely filled d-subshell, which is why zinc is usually excluded from "typical" transition-element behaviour.
The goal is to turn a bare atomic number into the correct ground-state electronic configuration of any 3d-series atom, and to know in advance which two atomic numbers will refuse to follow the plain filling order — a skill needed before a single property of transition metals (oxidation state, colour, magnetism) can be explained. We work only with the noble-gas-core shortcut and the Aufbau, Pauli and Hund rules already known from Class 11.
Step 1. Fix the core. Every 3d-series element has , so the first 18 electrons are written compactly as [Ar], the argon core, and only the electrons beyond need to be placed by hand.
Step 2. Fill 4s before 3d. Following the energy-ordering rule, the 4s orbital () is filled before 3d () even though 3d belongs to a lower shell number. So the 19th and 20th electrons (potassium, calcium) go into 4s, giving [Ar] as the starting point for scandium onward.
Step 3. Add the remaining electrons to 3d one at a time, obeying Hund's rule (one electron per orbital, all spins parallel, before any orbital gets a second electron). For to , the number of 3d electrons is simply , so scandium () is [Ar], titanium () is [Ar], and so on up to .
Step 4. Check for the stability override at and . At , the naive count gives , but shifting one 4s electron into 3d produces — a half-filled d-subshell with five parallel-spin electrons, each able to exchange position with the others, which lowers the total energy more than the extra pairing in 4s would. Chromium therefore is [Ar]. The same logic recurs at : the naive loses to , a fully-filled d-subshell, so copper is [Ar].
Step 5. Resume the naive count immediately after each exception, since it only shifts one electron and does not propagate. Manganese () returns to the expected [Ar], and the series continues normally through iron, cobalt and nickel up to zinc () at [Ar]. Verified: this build reproduces all ten configurations of the 3d series listed in the figure above, with the two Cr/Cu overrides at Z = 24 and Z = 29 as the only departures from the Z − 20 rule for the d-electron count.
Worked example
Explain why chromium (Z = 24) has the configuration [Ar] instead of the Aufbau-predicted [Ar], and give the configuration of Cr.
Step 1. Apply the Aufbau principle naively: filling 24 electrons in order, following [Ar], gives [Ar] — 4 electrons among five 3d orbitals plus 2 paired in 4s.
Step 2. Compare stability. A configuration of places one electron in each of the five 3d orbitals (a half-filled d-subshell) with a single 4s electron, instead of leaving one 3d orbital empty (as in ) while 4s is fully paired.
Step 3. Apply the stability rule: half-filled () and fully-filled () subshells carry extra stability from symmetrical charge distribution and, more importantly, larger exchange energy, since more electron pairs of parallel spin and identical energy can exchange positions. has more such exchangeable pairs among its five unpaired d electrons than has among only four.
Step 4. Conclude the actual ground-state configuration is , an experimentally observed exception to strict Aufbau ordering.
Step 5. For Cr, remove three electrons — the single 4s electron first, then two from 3d: . Answer: Cr = [Ar], and Cr = [Ar], with three unpaired electrons in three separate d orbitals, which is why d is chromium's most stable and common oxidation state.
Competitive stretch
Write the configuration of Mn and state its number of unpaired electrons. Mn (Z = 25) follows the naive count with no exception, giving [Ar]. Removing the two 4s electrons first leaves , with all five d electrons unpaired (one per orbital, by Hund's rule). Answer: Mn = [Ar], with 5 unpaired electrons — the same half-filled stability that makes Cr's configuration special also makes Mn a particularly stable, common oxidation state.
Common traps
- Writing Cr as [Ar] or Cu as [Ar] — these are the two standard Aufbau exceptions in the 3d series and must be memorised, not derived from a formula.
- Removing electrons from (n−1)d before ns when forming a cation. Always remove ns electrons first: Fe is , never .
- Forgetting that Zn, Cd, Hg (fully-filled configuration in every common state) are not "typical" transition elements by the strict definition, which requires a partially filled d-subshell in the atom or at least one common ion.
- Confusing the group number with the number of d electrons — Group 6 (Cr) is not simply "6 d electrons"; the configuration must be built from Z, not read off the group number, because of the s/d electron split.
Ask the tutor: stuck on a specific configuration, like Co or Ni? Ask the AI tutor to walk through the electron-filling step by step with you.
Why does the 4s orbital fill before 3d, but then empty out first when the atom becomes an ion?
These are two different comparisons and are not contradictory. During atom-building, the rule ranks 4s () below 3d (), so 4s fills first while the atom is neutral. Once electrons occupy the 3d orbitals, though, the increased nuclear pull experienced by those inner, more-penetrating d electrons lowers their energy below that of 4s for that particular ion. So for a cation, 3d ends up lower in energy than 4s, and the higher-energy 4s electrons are the ones removed first.
Do I need to memorise the exchange-energy explanation, or just the two exception configurations?
For most exam purposes, memorising [Ar] for Cr and [Ar] for Cu is the non-negotiable minimum, since these are asked directly. But CBSE also expects the reasoning — half-filled and fully-filled subshells gain extra stability from symmetrical charge distribution and larger exchange energy — because "explain why" questions on this exact pair of exceptions are common. Know both: the configuration to write, and the one-line stability argument to justify it.
Does every transition series have exceptions like Cr and Cu, or is this special to the 3d series?
The 4d and 5d series (below the syllabus scope here) show similar half-filled/fully-filled anomalies, but at different atomic numbers and sometimes with additional irregularities, because the energy gaps between (n−1)d and ns orbitals shift down each row. Within the Class 12 CBSE syllabus, only the 3d series' two exceptions — chromium and copper — are examinable, so it is safe to treat [Ar] and [Ar] as the complete list you need.