Look at the picture below: the left panel shows the two ways an electron makes magnetism (spin and orbital circulation), and the ruler on the right marks off magnetism in units of μB.
A single number is a lie detector for a lot of chemistry. Test whether you know why each statement holds or breaks.
A diamagnetic complex must have zero unpaired electrons
True — diamagnetism means every electron is paired, so n=0 and μso=0=0; there is no lone spin left to be attracted.
Two complexes with the same μ must have the same number of unpaired electrons
True for the spin-only regime — μ is a one-to-one function of n there, so equal μ forces equal n (though the metals and geometries can still differ).
A larger Δo always gives a larger magnetic moment
False — larger Δo favours pairing (low spin), which reduces the number of unpaired electrons and hence lowersμ.
Every d5 complex is high-spin with μ=5.92μB
False — d5 is high-spin (n=5) only with a weak field; a strong field (CN−) forces low-spin t2g5, giving n=1 and μ=1.73.
The spin-only formula works equally well for Nd3+ (a 4f ion)
False — for 4f ions the orbital angular momentum is not quenched, so spin-only fails; you need the full gJJ(J+1) expression with total angular momentum J.
A d10 ion is always diamagnetic regardless of ligand or geometry
True — all ten d-orbitals are full, every electron is paired, so n=0 no matter the field strength or shape.
Doubling n doubles μ
False — the relationship n(n+2) is curved, not linear; n=1 gives 1.73 but n=2 gives 2.83, not 3.46.
A paramagnetic reading proves the metal is a transition metal
False — any species with unpaired electrons is paramagnetic (e.g. O2, free radicals); paramagnetism alone says "unpaired electron present," not "transition metal."
Measured μ is the same at any temperature
False — by Curie's law the susceptibility scales as 1/T, so a paramagnet appears weaker when hotter; quoted μ values are the (nearly temperature-independent) effective moments extracted at a stated temperature.
Each line contains one flawed statement. Name the specific mistake, not just "it's wrong."
"Fe3+ is 3d5 because we remove three 3d electrons from 3d64s2."
Wrong removal order — you strip the two 4s electrons first, then only one 3d; the result 3d5 is right but the reasoning is not.
"μ=2.83μB means n=2.83 unpaired electrons."
n must be a whole number; 2.83=8=2(2+2), so this is n=2, and μ is never equal to n itself.
"[Ni(CN)4]2− is tetrahedral, so with d8 it has 2 unpaired electrons."
Strong-field CN− makes this d8 complex square planar, not tetrahedral; square-planar d8 is diamagnetic (n=0). See Square Planar vs Tetrahedral Geometry.
"Orbital angular momentum always adds to the spin moment, so real μ is always above spin-only."
In 3d complexes the orbital contribution is largely quenched by the ligand field, so measured values sit close to spin-only, not systematically above it.
"CN− is a weak-field ligand, so [Fe(CN)6]3− is high-spin."
CN− is a strong-field ligand near the top of the Spectrochemical Series; the complex is low-spin with n=1.
"Since μS=gS(S+1) uses S, the formula n(n+2) needs g=2."
The n(n+2) form comes from setting g=2 and S=n/2; it already bakes in g=2, so nothing extra is needed.
"All d5 ions are paramagnetic, so μ can never be zero for d5."
True that no d5 arrangement gives n=0 (odd electron count guarantees at least one unpaired), but the reasoning "d5 so paramagnetic" should cite the odd electron count, which is the real guarantee.
"A dimer of two Cu2+ (d9, one unpaired each) must show μ for two unpaired electrons."
If the two spins couple antiferromagnetically through a bridge, they cancel and μ drops toward zero; magnetic exchange coupling can hide unpaired electrons.
The formula is easy; the why is where understanding lives.
Why is the magnitude S(S+1) and not simply S
The full length of a quantum angular-momentum vector is S(S+1)ℏ (from the eigenvalue S(S+1)ℏ2 of L^2); only its shadow on one axis can reach S, so the true magnitude the moment tracks is larger.
Why do paired electrons contribute nothing to the magnetic moment
Two paired electrons spin in opposite directions, so their tiny magnetic fields cancel exactly, leaving no net moment — only lonely electrons survive.
Why is the spin-only formula so reliable for the first-row (3d) transition metals
The ligand field "freezes out" (quenches) the orbital motion, so spin dominates and the spin-only value matches experiment well.
Why does a strong-field ligand reduce the number of unpaired electrons
A large Δo makes pairing (cost P) cheaper than promoting to eg (cost Δo); when Δo>P electrons pair instead of spreading. See Hund's Rule and Pairing Energy.
Why can measuring μ reveal a complex's geometry
Different geometries force different orbital splittings and hence different n; e.g. square-planar d8 is diamagnetic while tetrahedral d8 is paramagnetic, so μ distinguishes them.
Why does the same ion Fe3+ give μ=5.92 with water but 1.73 with cyanide
The ligand, not the metal, sets Δo: weak-field water gives Δo<P (high-spin, n=5), strong-field cyanide gives Δo>P (low-spin, n=1).
Why must you use the ion's configuration, not the neutral atom's
Forming the complex removes electrons; counting the neutral atom's d-electrons overcounts, so you count d-electrons of the actual ion (e.g. Ni2+ is d8, not d10).
Why does the same Δo that controls magnetism also control colour
The gap Δo is the energy a photon must supply for a d–d transition; its size sets both the absorbed wavelength (colour) and the spin state (magnetism). See Color of Coordination Compounds.
Why can a compound with unpaired electrons still read a tiny μ
In bridged or multinuclear complexes the neighbouring spins can couple antiferromagnetically and partly cancel, so exchange coupling — not electron count — pulls μ down.
Boundaries are where careless rules snap. Walk each degenerate or extreme case deliberately.
Does a d0 ion (e.g. Ti4+, Sc3+) show any magnetic moment
No — with zero d-electrons there are no unpaired spins, so n=0 and the ion is diamagnetic.
Can high-spin and low-spin ever give the samen for a given d-count
Yes — for d1, d2, d3 (and d8, d9, d10) the filling is forced; high- and low-spin coincide, so Δo does not change n there.
For which octahedral d-counts does spin state actually matter
Only d4 through d7 — these are the configurations where you can choose to pair in t2g (cost P) or occupy eg (cost Δo), so the Δo vs P balance decides n.
Which dn arrangement gives the maximum possible unpaired electrons, and how many
High-spin d5 — all five orbitals singly occupied gives n=5, the largest for a single 3d set, so μ=5.92μB.
Is an odd d-electron count ever diamagnetic
No — an odd number of electrons cannot be fully paired, so at least one is always unpaired, guaranteeing paramagnetism.
What does μ=0 tell you, and what does it not tell you
It tells you all spins are effectively paired (n=0 or fully cancelled); it does not fix the geometry or d-count, since d0, d6 low-spin, square-planar d8, and antiferromagnetically coupled dimers can all read zero.
If measured μ lies between two integer-n values (say μ=4.5), what might be happening
An unquenched orbital contribution, a spin-state (high/low) equilibrium, or partial exchange coupling can push the observed value off the clean spin-only number.
How does temperature change the reading
By Curie's law the susceptibility varies as 1/T; you must measure at (or correct to) a stated temperature, otherwise a hotter sample looks like a weaker magnet even with the same n.
For a 4f lanthanide, why does spin-only fail and what replaces it
The buried 4f orbitals are shielded, so orbital motion is not quenched; spin and orbital combine into J and you use μ=gJJ(J+1)μB instead.
Recall One-line self-test
Cover everything and answer: "Why does measuring how hard a substance is pulled into a magnet tell a chemist the oxidation state and geometry of a metal?"
Because the pull measures unpaired electrons (n); n pins down the d-count and spin state, and those together fix the oxidation state and (via Δo vs P) the geometry — as long as no exchange coupling or unquenched orbital moment is confusing the reading.