CHEM 361 / Test Bank / Spectroscopy & Magnetism
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Test Bank — Unit 3

Electronic Spectroscopy & Magnetism

Practice problems drawn from Housecroft, Atkins, JD Lee, and others. Select an answer or click "Show Answer" to reveal the explanation.

UV-Vis Spectroscopy of Coordination Compounds

Questions 1–4
Housecroft & Sharpe, Chapter 20 Housecroft
UV-Vis absorption spectrum of a d-metal complex
Fig. 20.23 — Electronic absorption spectrum of a d-metal complex
Q1

Most transition metal complexes are brightly colored in solution. What is the fundamental electronic origin of color in these complexes?

  • a Electrons are emitted from the metal center, producing visible photons
  • b d–d transitions absorb specific wavelengths of visible light; the transmitted (complementary) color is observed
  • c The ligands fluoresce when coordinated to the metal
  • d Vibrational overtones of metal–ligand bonds fall in the visible region
Answer: (b)

Transition metal complexes are colored because d–d electronic transitions absorb photons in the visible region of the electromagnetic spectrum. The crystal field (or ligand field) splits the d orbitals into sets of different energy, and electrons can be promoted from the lower set to the upper set by absorbing light. The color we observe is the complementary color to the wavelengths absorbed.

Housecroft & Sharpe, Fig. 20.24 Housecroft
Absorption spectrum of [Ti(H2O)6]3+
Fig. 20.24 — UV-Vis spectrum of [Ti(H2O)6]3+
Q2

The complex [Ti(H2O)6]3+ appears purple and shows a single broad absorption band near 500 nm. What electronic transition is responsible for this absorption?

  • a t2g → eg: the single d electron is promoted across the Δoct splitting
  • b eg → t2g: an electron drops from the upper to the lower set
  • c A ligand π → metal d charge-transfer transition
  • d A metal 3d → 4s promotion
Answer: (a)

Ti3+ is a d1 ion. In an octahedral crystal field, the five d orbitals split into a lower t2g set and an upper eg set. The single electron occupies a t2g orbital and absorbs a photon of energy Δoct to be promoted to the eg set. This is the simplest possible d–d transition, giving a single absorption band whose energy directly measures Δoct.

Atkins & Shriver, Chapter 20 Atkins
Q3

Two important selection rules govern the intensity of d–d transitions. Which statement correctly describes the Laporte and spin selection rules?

  • a Laporte rule: transitions must change spin; spin rule: transitions must change parity (g → u)
  • b Laporte rule: only Δl = ±2 transitions are allowed; spin rule: ΔS = ±1 is required
  • c Laporte rule: transitions between states of the same parity (g → g) are forbidden; spin rule: transitions that change the total spin (ΔS ≠ 0) are forbidden
  • d Both rules only apply to tetrahedral complexes, not octahedral
Answer: (c)

The Laporte (parity) selection rule states that transitions between states of the same parity are forbidden: g → g and u → u are forbidden, while g → u is allowed. Since all d orbitals are gerade (g), d–d transitions are Laporte-forbidden in centrosymmetric complexes. The spin selection rule forbids transitions where the total spin quantum number changes (ΔS ≠ 0). Both rules explain why d–d bands are typically weak (low molar absorptivity).

Housecroft & Sharpe, Chapter 20 Housecroft
Q4

d–d transitions in octahedral complexes are Laporte-forbidden because they are g → g transitions. Yet octahedral complexes such as [Ti(H2O)6]3+ are still visibly colored. What mechanism allows these formally forbidden transitions to occur?

  • a Electron tunneling bypasses the selection rules entirely
  • b The magnetic dipole component of light drives the transition
  • c Spin–orbit coupling converts the d–d transition into a charge-transfer band
  • d Vibronic coupling: molecular vibrations temporarily destroy the center of symmetry, partially relaxing the Laporte rule
Answer: (d)

Vibronic coupling is the key mechanism. Asymmetric stretching vibrations of the metal–ligand bonds momentarily distort the octahedral geometry, temporarily removing the center of symmetry (inversion center). During these distorted configurations, the Laporte rule is partially relaxed, allowing d–d transitions to "steal" intensity. This is why octahedral d–d bands have low but nonzero molar absorptivities (typically ε ≈ 5–100 M−1cm−1).

Charge Transfer & Term Symbols

Questions 5–8
Housecroft & Sharpe, Fig. 20.32 Housecroft
Charge-transfer transitions in metal complexes
Fig. 20.32 — Schematic of charge-transfer transitions
Q5

Charge-transfer (CT) transitions in metal complexes produce bands that are typically much more intense than d–d bands. What is a CT transition, and why is it more intense?

  • a A CT transition moves an electron between two d orbitals on different metals; it is intense because two metal centers are involved
  • b A CT transition transfers electron density between the metal and a ligand; it is Laporte-allowed (g → u or u → g) and therefore much more intense
  • c A CT transition is a nuclear rearrangement that changes the oxidation state; intensity comes from the large nuclear displacement
  • d A CT transition involves core electrons, not valence electrons; core transitions are always fully allowed
Answer: (b)

A charge-transfer transition involves the movement of electron density between metal-centered and ligand-centered orbitals. Because these orbitals have different parity (metal d orbitals are gerade, ligand π or σ orbitals are ungerade), CT transitions are Laporte-allowed. This makes them orders of magnitude more intense than d–d transitions, with molar absorptivities typically ε > 1000 M−1cm−1, producing vivid colors.

JD Lee, Chapter 32 JD Lee
Q6

Two types of charge-transfer transitions are commonly observed in coordination compounds: LMCT and MLCT. Which of the following correctly distinguishes them with appropriate examples?

  • a LMCT: electron moves from metal to ligand (e.g., [Ru(bpy)3]2+); MLCT: electron moves from ligand to metal (e.g., MnO4)
  • b LMCT and MLCT are identical processes occurring in different solvents
  • c LMCT: electron moves from ligand to metal (e.g., MnO4, CrO42−); MLCT: electron moves from metal to ligand (e.g., [Ru(bpy)3]2+)
  • d LMCT occurs only in ionic compounds; MLCT occurs only in covalent compounds
Answer: (c)

In LMCT (ligand-to-metal charge transfer), electron density moves from a filled ligand orbital to an empty or partially filled metal orbital. This is common with high-oxidation-state metals and easily oxidized ligands (e.g., MnO4, CrO42−). In MLCT (metal-to-ligand charge transfer), electron density moves from a filled metal d orbital to an empty ligand π* orbital. MLCT is favored by low-oxidation-state metals and ligands with low-lying π* orbitals, such as bipyridine in [Ru(bpy)3]2+.

Housecroft & Sharpe, Chapter 20 Housecroft
Q7

KMnO4 is intensely purple despite Mn being in the +7 oxidation state (d0 configuration). Since there are no d electrons, d–d transitions are impossible. What is the origin of its color?

  • a LMCT: electrons transfer from filled oxygen 2p orbitals to empty Mn d orbitals, producing an intense, Laporte-allowed band
  • b MLCT: electrons transfer from filled Mn d orbitals to empty oxygen π* orbitals
  • c Intervalence charge transfer between two Mn centers in different oxidation states
  • d Spin-forbidden d–d transitions that gain intensity through spin–orbit coupling
Answer: (a)

In MnO4, Mn(VII) has a d0 configuration, so no d–d transitions are possible. The intense purple color arises from LMCT transitions: electrons are transferred from the filled oxygen 2p orbitals (ligand) to the empty Mn 3d orbitals (metal). Because this is a parity-allowed transition, the molar absorptivity is very high (ε > 2000 M−1cm−1), producing the characteristic deep purple color even at low concentrations.

Housecroft & Sharpe, Fig. 20.25 Housecroft
Tanabe-Sugano diagram
Fig. 20.25 — A Tanabe–Sugano diagram for a dn configuration
Q8

The figure above shows a Tanabe–Sugano diagram. What information does this diagram convey, and how is it used to interpret UV-Vis spectra of metal complexes?

  • a It plots oxidation state vs. coordination number to predict geometry
  • b It shows the relationship between bond length and bond energy for metal–ligand bonds
  • c It maps the variation of orbital energies with temperature
  • d It plots the energies of electronic states (term symbols) as a function of the ligand field strength Δoct/B, allowing prediction of absorption band positions and assignments
Answer: (d)

A Tanabe–Sugano diagram plots the energies of all electronic states arising from a given dn configuration as a function of the crystal field strength ratio Δoct/B, where B is the Racah interelectronic repulsion parameter. The ground state is taken as the energy zero (x-axis). By measuring the ratios of observed absorption band energies, one can locate the value of Δoct/B on the diagram, assign each band to a specific electronic transition, and extract both Δoct and B for the complex.

Magnetism

Questions 9–12
Housecroft & Sharpe, Chapter 20 Housecroft
Magnetic properties of transition metal complexes
Fig. 20.33 — Magnetic behavior of transition metal complexes
Q9

The spin-only magnetic moment formula is μs.o. = √(n(n+2)) BM, where n is the number of unpaired electrons. What is the predicted spin-only magnetic moment for a d5 high-spin octahedral complex?

  • a μ = √(3(5)) = 3.87 BM (3 unpaired electrons)
  • b μ = √(5(7)) = 5.92 BM (5 unpaired electrons)
  • c μ = √(1(3)) = 1.73 BM (1 unpaired electron)
  • d μ = 0 BM (all electrons are paired)
Answer: (b)

In a d5 high-spin octahedral complex (e.g., [Mn(H2O)6]2+), all five d electrons occupy separate orbitals with parallel spins according to Hund's rule: t2g3 eg2. This gives n = 5 unpaired electrons. Applying the spin-only formula: μs.o. = √(5 × 7) = √35 = 5.92 BM. This is the maximum possible spin-only moment for any dn configuration.

Atkins & Shriver, Chapter 20 Atkins
Q10

A chemist synthesizes a new Co3+ complex and wants to determine whether it is high-spin or low-spin. What experimental measurement would most directly distinguish between the two cases?

  • a Magnetic susceptibility measurement: high-spin Co3+ (d6) has 4 unpaired electrons (μ ≈ 4.9 BM), while low-spin has 0 (μ = 0)
  • b Measuring the melting point of the complex
  • c Determining the molecular weight by mass spectrometry
  • d Measuring the solubility in water
Answer: (a)

Magnetic susceptibility measurements (e.g., using a Gouy balance or SQUID magnetometer) directly report the number of unpaired electrons. For Co3+ (d6), the high-spin configuration is t2g4 eg2 with 4 unpaired electrons (μs.o. = √(4×6) = 4.90 BM), whereas the low-spin configuration is t2g6 with 0 unpaired electrons (μ = 0, diamagnetic). The difference is unambiguous and immediately diagnostic.

JD Lee, Chapter 18 JD Lee
Q11

Three principal types of magnetic behavior are observed in chemical substances: paramagnetism, diamagnetism, and ferromagnetism. Which description correctly distinguishes all three?

  • a Paramagnetic substances are repelled by a magnetic field; diamagnetic substances are attracted; ferromagnetic substances are unaffected
  • b All three types are attracted to a magnetic field but differ in their temperature dependence
  • c Diamagnetic: weakly repelled (all electrons paired); paramagnetic: weakly attracted (unpaired electrons, random alignment); ferromagnetic: strongly attracted (unpaired electrons with cooperative long-range alignment)
  • d Diamagnetic and paramagnetic apply only to metals; ferromagnetism applies only to nonmetals
Answer: (c)

Diamagnetic substances have all electrons paired and are weakly repelled by an external magnetic field. Paramagnetic substances contain unpaired electrons that align with the field, causing weak attraction; this alignment is lost when the field is removed. Ferromagnetic materials (Fe, Co, Ni) also have unpaired electrons, but neighboring spins align cooperatively in domains due to exchange interactions, producing strong, permanent magnetization that persists even after the external field is removed.

Housecroft & Sharpe, Chapter 20 Housecroft
High-spin and low-spin configurations for d-metal octahedral complexes
Fig. 20.10 — High-spin vs. low-spin d-electron configurations in octahedral complexes
Q12

The complex [Fe(H2O)6]2+ has an experimentally measured magnetic moment of μ ≈ 5.1 BM. Fe2+ is a d6 ion. Is this complex high-spin or low-spin, and how many unpaired electrons does it have?

  • a Low-spin with 0 unpaired electrons (μs.o. = 0 BM)
  • b High-spin with 4 unpaired electrons (μs.o. = 4.90 BM, consistent with ~5.1 BM)
  • c High-spin with 2 unpaired electrons (μs.o. = 2.83 BM)
  • d Low-spin with 2 unpaired electrons (μs.o. = 2.83 BM)
Answer: (b)

For Fe2+ (d6) in an octahedral field, the high-spin configuration is t2g4 eg2 with 4 unpaired electrons, giving μs.o. = √(4 × 6) = 4.90 BM. The low-spin configuration would be t2g6 with 0 unpaired electrons (μ = 0). The measured value of ~5.1 BM is close to the 4.90 BM prediction for 4 unpaired electrons, confirming the high-spin case. Water is a weak-field ligand, so Δoct is small and the high-spin configuration is favored.

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Electronic Spectroscopy & Magnetism