2.1.11Quantum Atomic Structure

Stability of half-filled and fully-filled subshells

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WHAT is going on?

The two physical reasons behind this stability are:

  1. Symmetrical distribution of electron density — a set of orbitals each with equal occupation (all singly or all doubly filled) gives a spherically symmetric, evenly-spread charge cloud that shields the nucleus uniformly and lowers repulsion.
  2. Exchange energy — a purely quantum-mechanical stabilization that grows with the number of parallel-spin electron pairs. This is the dominant reason.

WHY: Exchange energy from first principles

HOW to count the stabilization (approximate model). Count the number of distinct pairs of parallel-spin electrons. If a subshell has nn electrons all with parallel spin, the number of exchange pairs is:

Nex=(n2)=n(n1)2N_{\text{ex}} = \binom{n}{2} = \frac{n(n-1)}{2}

The d5d^5 vs d4d^4 argument (why 3d53d^5 wins)

For d5d^5 all five electrons are parallel (Hund's rule), so among the 3d3d electrons: Nex(3d3d)=(52)=10 exchange pairsN_{\text{ex}}(3d\text{–}3d) = \binom{5}{2} = 10 \text{ exchange pairs}

Compare Chromium's two candidate configurations. Below we count within-3d3d pairs (the biggest, most comparable contribution):

Config 3d3d spins 4s4s spins 3d3d3d3d parallel pairs
[Ar]3d44s2[Ar]3d^4 4s^2 ↑↑↑↑ (4 up) ↑↓ (paired) (42)=6\binom{4}{2}=6
[Ar]3d54s1[Ar]3d^5 4s^1 ↑↑↑↑↑ (5 up) ↑ (1 up) (52)=10\binom{5}{2}=10

Going 3d44s23d54s13d^4 4s^2 \to 3d^5 4s^1 gains 4 extra 3d3d3d3d exchange pairs (106=410-6=4), i.e. 4K3d,3d\approx -4K_{3d,3d}.

Similarly for Cu: 3d94s23d104s13d^9 4s^2 \to 3d^{10} 4s^1 completes the dd subshell (fully-filled d10d^{10}), maximizing both symmetry and pairing stabilization.


Figure — Stability of half-filled and fully-filled subshells

Worked examples



Active recall

Recall Test yourself (hover/expand)
  • Which three p/d/fp/d/f occupations count as "half-filled"? → p3,d5,f7p^3, d^5, f^7.
  • Formula for number of exchange pairs among nn parallel electrons? → (n2)=n(n1)2\binom{n}{2}=\frac{n(n-1)}{2}.
  • Is the exchange integral KK the same for every pair? → No — KijK_{ij} depends on orbital overlap (3d3d3d3d3d \ne 3d4s4s); single-KK is an approximation.
  • Why does Cr adopt 3d54s13d^5 4s^1? → gains 4 extra 3d3d3d3d exchange pairs + symmetry, and 3d4s3d\approx4s energy.
  • Two physical reasons for extra stability? → symmetric charge distribution + exchange energy.
Recall Feynman: explain to a 12-year-old

Imagine electrons are kids on swings, and identical kids (same spin) love to swap swings. Every possible swap makes the whole playground a little happier (lower energy). But swaps between kids on nearby swings help more than swaps between kids far apart — so not every swap is worth the same. When each swing has exactly one kid facing the same way, there are LOTS of possible swaps, so the playground is super happy — that's a "half-filled" shell. Sometimes an atom will even move one kid from a nearby playground just to make more swaps possible. That's why Chromium and Copper "cheat" the normal seating order!


Connections


Which subshell occupations are "half-filled" and extra stable?
p3p^3, d5d^5, f7f^7 (one electron per orbital, all parallel spins).
Which subshell occupations are "fully-filled"?
p6p^6, d10d^{10}, f14f^{14} (two electrons per orbital).
What are the TWO physical reasons for half/full-filled stability?
Symmetrical charge distribution + exchange energy (the dominant one).
Formula for number of exchange pairs among nn parallel-spin electrons?
(n2)=n(n1)2\binom{n}{2} = \dfrac{n(n-1)}{2}.
Is the exchange integral the same for every same-spin pair?
No — KijK_{ij} depends on spatial overlap of orbitals i,ji,j; the single-KK / (n2)K\binom{n}{2}K form is an approximation. Exact: E=i<jKijE=-\sum_{i<j}K_{ij}.
Electronic configuration of Cr (Z=24Z=24)?
[Ar]3d54s1[Ar]3d^5 4s^1 (not 3d44s23d^4 4s^2).
Electronic configuration of Cu (Z=29Z=29)?
[Ar]3d104s1[Ar]3d^{10} 4s^1 (not 3d94s23d^9 4s^2).
How many extra 3d–3d exchange pairs does Cr gain going 3d44s23d54s13d^4 4s^2 \to 3d^5 4s^1?
106=410 - 6 = 4 pairs, i.e. 4K3d,3d\approx -4K_{3d,3d} (ignoring smaller cross 3d3d4s4s terms).
Why is exchange energy negative (stabilizing)?
Indistinguishable same-spin electrons can swap positions; each swap lowers energy by its KijK_{ij}.
Why can an atom promote an electron from 4s4s to 3d3d?
3d3d and 4s4s energies are very close, so exchange + symmetry gains can outweigh the small cost.
Why is nitrogen's first ionization energy higher than oxygen's?
N has a stable half-filled 2p32p^3; removing an electron disrupts it, costing extra energy.
Does the half/full-filled anomaly happen for ALL elements?
No — only when nsns and (n1)d(n-1)d energies are close enough for exchange gain to win.

Concept Map

gives

gives

arises from

arises from

allows swaps

quantified by

summed over

counts as binom n 2

maximized at

overrides filling order

reduced by

Electron repulsion in subshell

Bonus stability

Half-filled p3 d5 f7

Fully-filled p6 d10 f14

Symmetrical charge density

Exchange energy dominant

Electrons indistinguishable

Exchange integral Kij

Pairs of parallel spins

Stabilization -n n-1 /2 K

Anomalies Cr and Cu

Hinglish (regional understanding)

Intuition Hinglish mein samjho

Dekho, electrons ek subshell mein ek doosre ko repel karte hain, lekin ek chhupa hua quantum bonus bhi milta hai — jise exchange energy kehte hain. Jab do electrons ka spin same hota hai (dono up ya dono down), toh woh aapas mein jagah swap kar sakte hain, aur har possible swap se poore atom ki energy thodi si kam ho jaati hai. Jitne zyada parallel-spin electrons, utne zyada swaps, utni zyada stability. Isiliye half-filled (d5d^5) aur fully-filled (d10d^{10}) configurations extra stable hote hain.

Ek important baat: har swap ki energy ek jaisi nahi hoti. Exchange integral KijK_{ij} do orbitals ke overlap par depend karta hai — 3d3d3d3d pair ka KK alag, 3d3d4s4s pair ka alag, aur 4s4s4s4s ka alag. Textbook wala neat formula (n2)K\binom{n}{2}K ek average KK maan leta hai — intuition aur exam ke liye badhiya, par yaad rakhna asli energy i<jKij-\sum_{i<j}K_{ij} hoti hai.

Number of swaps count karna easy hai: nn parallel electrons mein (n2)=n(n1)2\binom{n}{2}=\frac{n(n-1)}{2} pairs. Chromium mein dekho — 3d44s23d^4 4s^2 mein 4 up 3d3d electrons (6 pairs), aur 3d54s13d^5 4s^1 mein 5 up 3d3d electrons (10 pairs). Yaani 4 extra 3d3d3d3d exchange pairs 4K3d,3d\approx -4K_{3d,3d}! (3d3d4s4s cross terms bhi hote hain par chote hote hain kyunki overlap kam hai.) Isiliye Cr apni normal filling tod ke 3d54s13d^5 4s^1 chunta hai. Same Copper ke saath — 3d104s13d^{10} 4s^1, fully-filled d10d^{10} ke liye. Aur yeh cheating tabhi hoti hai jab 3d3d aur 4s4s ki energy close ho. Exam mein Cr, Cu ki config + exchange energy reason — high-yield 80/20 point hai!

Go deeper — visual, from zero

Test yourself — Quantum Atomic Structure

Connections