Q.Predict the number of unpaired electrons in the square planar [Pt(CN)4]2− ion.
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Magnetic Moment Calculation
From a Paperclip to a Magnet: The Intuition
You already know that a magnet can pick up iron nails. But what is actually happening inside that nail when it gets near the magnet? And why does a plastic comb, rubbed on hair, pick up tiny bits of paper — but never iron filings?
The answer lies in magnetization — the process by which a material becomes magnetic.
Think of a piece of iron as a chaotic crowd of tiny compass needles. Each needle is an atomic magnetic moment (a tiny magnet, arising from the spin of electrons). In unmagnetized iron, these needles point in random directions. Their magnetic effects cancel out, so the iron as a whole shows no net magnetism.
Now bring a strong magnet close. Its magnetic field acts like a command: "Line up!" The tiny compass needles inside the iron start rotating, aligning themselves with the external field. The more they align, the stronger the iron's own magnetic field becomes. This alignment is magnetization.
Magnetization is not the same as inducing a current. It is a purely magnetic reorientation of atomic dipoles inside a material.
The Precise Definition
Magnetization (M) is the net magnetic dipole moment per unit volume of a material. It tells you how strongly a material is magnetized — how many tiny atomic magnets are aligned, and in which direction.
If a material has N atoms per unit volume, each with an average magnetic moment μavg, then:
M=Nμavg
The SI unit of M is amperes per metre (A/m). Why? Because a magnetic dipole moment has units of A·m², and dividing by volume (m³) gives A/m.
M=volumetotal magnetic dipole moment
How Magnetization Connects to the Magnetic Field
When a material gets magnetized, it produces its own magnetic field. The total magnetic field B inside the material is the sum of:
- The external applied field H (caused by free currents, like the current in a solenoid)
- The material's response — the magnetization M
The fundamental relation is:
B=μ0(H+M)
where μ0=4π×10−7T⋅m/A is the permeability of free space.
Do not confuse H (magnetic field intensity, or "magnetizing field") with B (magnetic flux density). H is what you apply; M is what the material does; B is the total field you measure.
The Three Kinds of Magnetic Materials
Not all materials respond the same way to an external field. The magnetization M is proportional to H for most materials (at least for small fields):
M=χmH
where χm is the magnetic susceptibility — a dimensionless number that tells you how easily a material magnetizes.
| Material Type | χm | Behaviour | Example |
|---|---|---|---|
| Diamagnetic | Small and negative (≈−10−5) | Weakly repelled by a magnet; M opposes H | Water, copper, bismuth |
| Paramagnetic | Small and positive (≈10−5 to 10−3) | Weakly attracted; M aligns with H | Aluminium, oxygen gas |
| Ferromagnetic | Large and positive (≫1) | Strongly attracted; M can be huge and persists even after H is removed | Iron, nickel, cobalt |
Why this formula?
Magnetic Moment Calculation: Why the Formula Holds
Let's build this from first principles — understanding the why before the formula.
1. What is Magnetic Moment?
A magnetic moment (μ) is a measure of the strength and orientation of a magnet or current loop. It tells us how strongly an object will interact with an external magnetic field.
The core idea: any moving charge creates a magnetic field. A loop of current is like a tiny bar magnet — its magnetic moment quantifies this.
2. The Fundamental Formula: Current Loop
The Setup
Consider a planar loop of wire carrying a steady current I, enclosing an area A.
Why μ=IA?
Step 1: Force on a moving charge
A charge q moving with velocity v in a magnetic field B experiences:
F=q(v×B)
Step 2: Torque on a current loop
For a rectangular loop of sides a and b (A=ab), placed in a uniform B:
- Current I means charge flows. On side of length a, the force magnitude is F=IaB (since I=tq and v=ta).
- These forces on opposite sides form a couple (equal, opposite, not collinear).
- Torque τ=force×perpendicular distance=(IaB)×(bsinθ)
Step 3: Recognize the pattern
τ=I(ab)Bsinθ=IABsinθ
This looks exactly like:
τ=μBsinθ
Comparing, we identify:
μ=IA
Why this works: The torque on a current loop is proportional to the current and the area — this product naturally defines the magnetic moment.
3. For a Single Moving Charge (Orbital Magnetic Moment)
The Setup
An electron of charge −e moves in a circular orbit of radius r with speed v.
Why μ=2evr?
Step 1: Treat orbit as a current loop
- Time for one revolution: T=v2πr
- Current (charge per unit time): I=Te=2πrev
Step 2: Apply μ=IA
- Area of orbit: A=πr2
- So: μ=(2πrev)(πr2)=2evr
Step 3: Express in terms of angular momentum
- Orbital angular momentum: L=mvr
- Therefore: μ=2meL
Why this matters: The magnetic moment is directly proportional to angular momentum. The factor 2me is called the gyromagnetic ratio — it links mechanics to magnetism.
4. For a Solenoid (Many Turns)
The Setup
A solenoid of N turns, length l, carrying current I, cross-sectional area A.
Why μ=NIA? …
The key idea is that the magnetic moment depends on the number of unpaired electrons, which in turn depends on the metal's oxidation state, geometry, and ligand field splitting.
Step 1: Determine the oxidation state and electron configuration of Pt.
Pt is in group 10. In [Pt(CN)4]2−, each CN⁻ is −1, so Pt has oxidation state +2.
Pt(0): [Xe]4f145d96s1
Pt(II): remove two electrons (from 6s first), giving [Xe]4f145d8.
Step 2: Consider the geometry and ligand field. …
The key is to determine the oxidation state of Pt, then its d-electron count, and finally the crystal field splitting in a square planar geometry. For [Pt(CN)4]2−, Pt is in the +2 state with a d8 configuration, and the strong-field CN⁻ ligands cause pairing of all electrons, giving zero unpaired electrons.
Why This Approach Works
Magnetic moment tells us about unpaired electrons. To predict them, we need two things: the number of d-electrons on the central metal ion, and how those electrons arrange themselves under the influence of the ligands.
Square planar geometry is a special case. It arises most commonly for d8 metal ions with strong-field ligands — think Ni²⁺, Pd²⁺, Pt²⁺. The crystal field splitting in a square planar complex is essentially an extreme version of octahedral splitting where two trans ligands are removed, causing one set of d-orbitals to rise dramatically in energy. The result is a large energy gap between the lower and upper d-orbitals, forcing electrons to pair up.
CN⁻ is a strong-field ligand (high up in the spectrochemical series). So we expect maximum pairing.
Let’s walk through it step by step.
- Find the oxidation state of platinum. The complex ion is [Pt(CN)4]2−. Each CN⁻ ligand carries a –1 charge. Let the oxidation state of Pt be x.
x+4(−1)=−2⇒x−4=−2⇒x=+2
So platinum is in the +2 oxidation state.
-
Determine the d-electron count for Pt(II).
Platinum (Pt) has atomic number 78. Its ground-state electron configuration is [Xe]4f145d96s1.
When Pt loses two electrons to become Pt²⁺, it loses the 6s electron first, then one 5d electron.
So Pt²⁺ has the configuration [Xe]4f145d8.
That’s a d8 system.
-
Recall the crystal field splitting pattern for square planar geometry.
In a square planar complex, the d-orbital energies (from lowest to highest) are:
- dxz,dyz (degenerate, lowest)
- dz2 (slightly higher)
- dxy (higher still)
- dx2−y2 (highest, by a large margin)
The energy gap between the dxy and dx2−y2 orbitals is very large — comparable to or larger than the pairing energy for a d8 ion with strong-field ligands.
For square planar d8 with strong-field ligands, the splitting is so large that all eight electrons occupy the four lower orbitals, leaving the dx2−y2 orbital empty.
-
Fill the electrons according to Hund’s rule and the Aufbau principle. …
Method: Crystal Field Theory (CFT) for Square Planar Geometry
Why this method?
Square planar complexes arise from d8 configurations (like Pt2+) when the ligand field is very strong. CFT explains how d-orbital energies split, which directly tells us the electron arrangement and number of unpaired electrons.
Step 1: Determine the oxidation state and d-electron count
- Platinum (Pt) is in Group 10, atomic number 78.
- Each cyanide ligand (CN−) has a charge of −1. Four ligands give −4.
- Complex charge is 2−.
- Let oxidation state of Pt be x:
x+4(−1)=−2⇒x=+2
- Pt2+: neutral Pt has [Xe]4f145d96s1. Removing two electrons (from 6s first) gives 5d8.
- d8 configuration.
Step 2: Recall the square planar d-orbital splitting
For a strong-field square planar complex, the energy order (lowest to highest) is:
dxz,dyz<dz2<dxy<dx2−y2
- The gap between dxy and dx2−y2 is very large (strong field).
- This forces pairing of electrons in the lower orbitals.
Step 3: Fill the d-orbitals (Aufbau + Hund's rule)
For d8 in strong-field square planar: …
Here are the most common mistakes students make when calculating magnetic moments and unpaired electrons for square planar complexes like [Pt(CN)4]2−, along with how to avoid each.
1. Forgetting to Check the Oxidation State of the Metal
The Mistake:
Students jump straight to the geometry without first finding the oxidation number of platinum. This leads to using the wrong dn configuration.
How to Avoid:
Always start with the charge balance.
- Ligand charge: Each CN− is −1, so total from 4 ligands = −4.
- Complex charge: −2.
- Let oxidation state of Pt be x:
x+(−4)=−2⇒x=+2
So Pt is in the +2 oxidation state.
2. Using the Wrong Electronic Configuration for the Metal Ion
The Mistake:
Assuming Pt has the same configuration as Ni or Pd, or forgetting that Pt is a 5d series element.
How to Avoid:
- Pt atomic number = 78.
- Neutral Pt: [Xe]4f145d96s1 (or 5d86s2 — but the 5d96s1 is more stable).
- For Pt2+, remove two electrons — remove the 6s electrons first:
Pt2+:[Xe]4f145d8
So the d-electron count is d8.
3. Assuming Square Planar Always Means Low-Spin
The Mistake:
Students think all square planar complexes are diamagnetic (no unpaired electrons). This is not always true — it depends on the metal and ligand field strength.
How to Avoid:
- For d8 ions, square planar geometry is strongly favoured by strong-field ligands like CN−.
- Strong field → large splitting → electrons pair up in the lower orbitals.
- For Pt2+ (a 5d metal), the splitting is very large due to relativistic effects.
- Result: All 8 electrons are paired → zero unpaired electrons.
4. Confusing Square Planar with Tetrahedral Geometry
The Mistake:
Some students treat [Pt(CN)4]2− as tetrahedral (common for d8 with weak-field ligands like Cl−), leading to a different d-orbital splitting and wrong unpaired electron count.
How to Avoid:
- Pt2+ with strong-field ligands like CN− always forms square planar complexes.
- Tetrahedral d8 would have 2 unpaired electrons; square planar d8 has 0 unpaired electrons.
- Memorise: Ni2+ can be tetrahedral or square planar; Pt2+ and Pd2+ are always square planar.
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Showing the 12 most recent of 15 on this concept.
- CBSE 2026Set ANNUAL1 markQ.Write the formula for calculating 'spin only' magnetic moment.
›Reveal solutionSolution
The spin-only formula estimates a transition metal ion's magnetic moment purely from its number of unpaired electrons, ignoring orbital contribution.
…
- CBSE 2026Set ANNUAL1 markQ.Give one example of a complex having tetrahedral geometry and paramagnetic in nature.
›Reveal solutionSolution
[NiCl4]2− is the standard example of a tetrahedral, paramagnetic complex, arising from sp3 hybridisation of Ni2+ with the weak-field Cl− ligand.
Why [NiCl4]2− fits
Ni has configuration [Ar]3d84s2; in Ni2+, this becomes 3d8. Cl− is a weak-field ligand (low in the spectrochemical series), so it does not force pairing of the 3d electrons. With four ligands and no d-orbital freed by pairing, nickel uses one 4s and three 4p orbitals — sp3 hybridisation — giving a **tetrahedr …
- CBSE 2026Set ANNUAL1 markQ.According to VBT, which one has the highest paramagnetic character? [Cr(H2O)6]3+ or [Fe(H2O)6]2+
›Reveal solutionSolution
Counting unpaired d-electrons for each ion under VBT shows Fe2+ (d6, high-spin, 4 unpaired) is more paramagnetic than Cr3+ (d3, always 3 unpaired).
[Cr(H2O)6]3+
Cr (Z=24) is [Ar]3d54s1; Cr3+ removes 3 electrons to give 3d3. With only 3 electrons for the three t2g orbitals, Hund's rule places one electron in each — t2g3 — giving 3 unpaired electrons, regardless of whether the ligand is weak- or strong-field (there's no way to pair up 3 electrons across 3 orbitals to reduce this further).
[Fe(H2O)6]2+
…
- CBSE 2026Set ANNUAL1 markQ.Write True or False: Value of magnetic moment of a divalent ion in aqueous solution having atomic number 25, will be 5.92 B.M.
›Reveal solutionSolution
Mn2+ has 5 unpaired electrons, giving a spin-only moment of 5.92 B.M., so the statement is true.
Atomic number 25 = manganese, [Ar] 3d5 4s2. The divalent ion Mn2+ = [Ar] 3d5, which has 5 unpaired electrons.
…
- CBSE 2026Set ANNUAL1 markMCQQ.Which one of the following metal ions is likely to have a magnetic moment of 1.73 BM?(a) Fe²⁺(b) Mn²⁺(c) Cr²⁺(d) Cu²⁺
›Reveal solutionSolution
Using μ = √(n(n+2)) BM, 1.73 BM means n = 1 unpaired electron; Cu²⁺ (d⁹) is the only ion with one unpaired electron — option (D).
The spin-only magnetic moment is μ=n(n+2) BM, where n is the number of unpaired electrons. A value of 1.73 BM gives 1(1+2)=3=1.73, so n=1 unpaired electron.
Now count unpaired electrons for each ion:
- Fe2+: 3d6 → 4 unpaired (μ≈4.9 BM). …
- CBSE 2025Set JZ1 markMCQQ.Magnetic moment of a bivalent ion in aqueous solution will be, if its atomic number is 25(a) 1.73 BM(b) 2.83 BM(c) 4.96 BM(d) 5.92 BM
›Reveal solutionSolution
Mn2+ (3d5) has 5 unpaired electrons, so μ=5(5+2)=5.92 BM — option (d).
Concept. The magnetic moment of a transition-metal ion depends only on the number of unpaired d-electrons (n), through the spin-only formula μ=n(n+2) BM.
Step 1 — identify the ion. Atomic number 25 → manganese (Mn), configuration [Ar]3d54s2. A bivalent ion Mn2+ loses the two 4s electrons: Mn2+=[Ar]3d5.
…
- CBSE 2025Set ANNUAL1 markMCQQ.The spin magnetic moment of Co3+ ion is:(a) sqrt(3) BM(b) sqrt(8) BM(c) sqrt(15) BM(d) sqrt(24) BM
›Reveal solutionSolution
Co3+ has the configuration [Ar]3d6; in the high-spin (free-ion) state this places 4 electrons unpaired, giving a spin-only magnetic moment of √(n(n+2)) = √24 BM.
Cobalt (Z = 27) has ground state configuration [Ar]3d7 4s2. Removing 3 electrons to form Co3+ removes the two 4s electrons first and then one 3d electron, giving Co3+: [Ar]3d6.
Filling the five d orbitals with 6 electrons by Hund's rule (maximum multiplicity, i.e., high-spin, as would apply to the free gaseous ion or in a weak field):
↑↓ ↑ ↑ ↑ ↑ → one orbital doubly occupied, four orbitals singly occupied → 4 unpaired electrons (n = 4).
…
- CBSE 2025Set ANNUAL1 markMCQQ.Which of the following is a paramagnetic complex?(a) [Ni(H2O)6]2+(b) [Ni(CO)4](c) [Zn(NH3)4]2+(d) [Co(NH3)6]
›Reveal solutionSolution
Ni2+ (d8) with the weak-field ligand H2O keeps 2 electrons unpaired; the other three complexes all have a d10 or strong-field-paired d-count and are diamagnetic.
[Ni(H₂O)₆]²⁺: Ni²⁺ is d⁸; H₂O is a weak-field ligand and cannot force pairing, so 2 electrons remain unpaired — paramagnetic (octahedral, sp³d² outer-orbital complex).
[Ni(CO)₄]: here nickel is in the zero oxidation state, Ni(0), configuration 3d¹⁰4s⁰ — a completely filled d-subshell regardless of ligand field, so it is diamagnetic (sp³, tetrahedral).
[Zn(NH₃)₄]²⁺: Zn²⁺ is always 3d¹⁰ (fully filled) in its only common oxidation state, so it is diamagnetic (sp³, tetrahedral) irrespective of the ligand.
…
- CBSE 2024Set ANNUAL1 markMCQQ.The magnetic moment of Mn+2 in aqueous solution is –(a) 2.84 B.M(b) 3.87 B.M(c) 4.90 B.M(d) 5.92 B.M
›Reveal solutionSolution
Mn²⁺ has a half-filled d⁵ configuration with 5 unpaired electrons, and the spin-only formula gives a magnetic moment of 5.92 B.M.
Mn2+ has the configuration [Ar]3d5 — a half-filled d-subshell, with all 5 electrons unpaired (by Hund's rule, each of the 5 d-orbitals holds one electron).
Using the spin-only formula:
μ=n(n+2) B.M.,n=5
…
- CBSE 2023Set ANNUAL1 markQ.Calculate the spin only magnetic moment of M2+(aq) ion (Z=27).
›Reveal solutionSolution
Z=27 corresponds to cobalt; Co2+(aq) has the configuration 3d7 with 3 unpaired electrons, giving a spin-only magnetic moment of 15≈3.87 BM.
Identify the ion: Z=27 is cobalt (Co), with ground-state configuration [Ar]3d74s2. Removing 2 electrons (always from 4s first) to form Co2+ gives:
Co2+:[Ar]3d7
Count unpaired electrons: Distributing 7 electrons among the five 3d orbitals following Hund's rule (each orbital singly filled first, before pairing) for the aqua ion (a weak-field, high-spin case):
↑↓ ↑↓ ↑ ↑ ↑
…
- CBSE 2020Set 56/2/11 markMCQQ.Total number of unpaired electrons present in Co3+ (Atomic number = 27) is (A) 2 (B) 7 (C) 3 (D) 5
›Reveal solutionSolution
Cobalt loses three electrons to form Co3+, leaving an electronic configuration of [Ar]3d6. In the d6 configuration, pairing depends on ligand field strength, but the question asks for the ground-state free ion, which follows Hund's rule and has 4 unpaired electrons.
The number of unpaired electrons in a transition metal ion determines its magnetic properties. To find this, we need the electronic configuration of the ion and then apply Hund's rule of maximum multiplicity.
Understanding the Configuration
Cobalt has atomic number 27. The neutral atom's electronic configuration is:
[Ar]3d74s2
When cobalt forms Co3+, it loses three electrons. Electrons are always removed from the outermost shell first—both 4s electrons go first, then one 3d electron:
Co3+:[Ar]3d6
Applying Hund's Rule
The five 3d orbitals can hold up to 10 electrons. With 6 electrons to place, Hund's rule tells us to:
- Maximize unpaired electrons first by placing one electron in each orbital with parallel spin.
- Then pair up any remaining electrons.
Let me show the filling pattern for 3d6:
dxy dyz dzx dx2−y2 dz2 ↑↓ ↑ ↑ ↑ ↑ The first five electrons occupy all five orbitals singly (all spin-up). The sixth electron must pair with one of them.
Result: 4 unpaired electrons and 1 paired set. …
- CBSE 2019Set ANNUAL1 markQ.Calculate the magnetic moment of a divalent ion in aqueous solution if its atomic number is 25.
›Reveal solutionSolution
The divalent ion of element 25 is Mn2+, a 3d5 ion with all five d-orbitals singly occupied; the spin-only formula then gives μ≈5.92 BM.
Element with atomic number 25 is manganese (Mn): [Ar]3d54s2.
Forming the divalent ion Mn2+ removes the two 4s electrons first:
Mn2+: [Ar]3d5
By Hund's rule, all five 3d electrons occupy the five d-orbitals singly (maximum multiplicity), giving n=5 unpaired electrons.
…
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