3.4.12 · D5Coordination Chemistry

Question bank — Magnetic moments of complexes

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Before the traps, this page builds every symbol it will test you on — so no reveal ever uses a term you have not yet met.


The toolkit — every symbol earned first

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 .

Figure — Magnetic moments of complexes
Figure — Magnetic moments of complexes
Figure — Magnetic moments of complexes

True or false — justify

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 and ; there is no lone spin left to be attracted.
Two complexes with the same must have the same number of unpaired electrons
True for the spin-only regime — is a one-to-one function of there, so equal forces equal (though the metals and geometries can still differ).
A larger always gives a larger magnetic moment
False — larger favours pairing (low spin), which reduces the number of unpaired electrons and hence lowers .
Every complex is high-spin with
False — is high-spin () only with a weak field; a strong field () forces low-spin , giving and .
The spin-only formula works equally well for (a ion)
False — for ions the orbital angular momentum is not quenched, so spin-only fails; you need the full expression with total angular momentum .
A ion is always diamagnetic regardless of ligand or geometry
True — all ten -orbitals are full, every electron is paired, so no matter the field strength or shape.
Doubling doubles
False — the relationship is curved, not linear; gives but gives , not .
A paramagnetic reading proves the metal is a transition metal
False — any species with unpaired electrons is paramagnetic (e.g. , free radicals); paramagnetism alone says "unpaired electron present," not "transition metal."
Measured is the same at any temperature
False — by Curie's law the susceptibility scales as , so a paramagnet appears weaker when hotter; quoted values are the (nearly temperature-independent) effective moments extracted at a stated temperature.

Spot the error

Each line contains one flawed statement. Name the specific mistake, not just "it's wrong."

" is because we remove three electrons from ."
Wrong removal order — you strip the two electrons first, then only one ; the result is right but the reasoning is not.
" means unpaired electrons."
must be a whole number; , so this is , and is never equal to itself.
" is tetrahedral, so with it has 2 unpaired electrons."
Strong-field makes this complex square planar, not tetrahedral; square-planar is diamagnetic (). See Square Planar vs Tetrahedral Geometry.
"Orbital angular momentum always adds to the spin moment, so real is always above spin-only."
In complexes the orbital contribution is largely quenched by the ligand field, so measured values sit close to spin-only, not systematically above it.
" is a weak-field ligand, so is high-spin."
is a strong-field ligand near the top of the Spectrochemical Series; the complex is low-spin with .
"Since uses , the formula needs ."
The form comes from setting and ; it already bakes in , so nothing extra is needed.
"All ions are paramagnetic, so can never be zero for ."
True that no arrangement gives (odd electron count guarantees at least one unpaired), but the reasoning " so paramagnetic" should cite the odd electron count, which is the real guarantee.
"A dimer of two (, one unpaired each) must show for two unpaired electrons."
If the two spins couple antiferromagnetically through a bridge, they cancel and drops toward zero; magnetic exchange coupling can hide unpaired electrons.

Why questions

The formula is easy; the why is where understanding lives.

Why is the magnitude and not simply
The full length of a quantum angular-momentum vector is (from the eigenvalue of ); only its shadow on one axis can reach , 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 () 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 makes pairing (cost ) cheaper than promoting to (cost ); when electrons pair instead of spreading. See Hund's Rule and Pairing Energy.
Why can measuring reveal a complex's geometry
Different geometries force different orbital splittings and hence different ; e.g. square-planar is diamagnetic while tetrahedral is paramagnetic, so distinguishes them.
Why does the same ion give with water but with cyanide
The ligand, not the metal, sets : weak-field water gives (high-spin, ), strong-field cyanide gives (low-spin, ).
Why must you use the ion's configuration, not the neutral atom's
Forming the complex removes electrons; counting the neutral atom's -electrons overcounts, so you count -electrons of the actual ion (e.g. is , not ).
Why does the same that controls magnetism also control colour
The gap is the energy a photon must supply for a 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
In bridged or multinuclear complexes the neighbouring spins can couple antiferromagnetically and partly cancel, so exchange coupling — not electron count — pulls down.

Edge cases

Boundaries are where careless rules snap. Walk each degenerate or extreme case deliberately.

Does a ion (e.g. , ) show any magnetic moment
No — with zero -electrons there are no unpaired spins, so and the ion is diamagnetic.
Can high-spin and low-spin ever give the same for a given -count
Yes — for , , (and , , ) the filling is forced; high- and low-spin coincide, so does not change there.
For which octahedral -counts does spin state actually matter
Only through — these are the configurations where you can choose to pair in (cost ) or occupy (cost ), so the vs balance decides .
Which arrangement gives the maximum possible unpaired electrons, and how many
High-spin — all five orbitals singly occupied gives , the largest for a single set, so .
Is an odd -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 tell you, and what does it not tell you
It tells you all spins are effectively paired ( or fully cancelled); it does not fix the geometry or -count, since , low-spin, square-planar , and antiferromagnetically coupled dimers can all read zero.
If measured lies between two integer- values (say ), 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 ; you must measure at (or correct to) a stated temperature, otherwise a hotter sample looks like a weaker magnet even with the same .
For a lanthanide, why does spin-only fail and what replaces it
The buried orbitals are shielded, so orbital motion is not quenched; spin and orbital combine into and you use 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 (); pins down the -count and spin state, and those together fix the oxidation state and (via vs ) the geometry — as long as no exchange coupling or unquenched orbital moment is confusing the reading.


Connections

  • Crystal Field Theory — the splitting behind every high/low-spin trap here.
  • Spectrochemical Series — tells you which ligand gives large or small .
  • Electronic Configuration of d-block ions — the source of every -count.
  • Square Planar vs Tetrahedral Geometry — the geometry traps in the edge cases.
  • Hund's Rule and Pairing Energy — the vs tug-of-war deciding .
  • Color of Coordination Compounds — same , two observables.