§5.1 §5.1 The Dewar-Chatt-Duncanson Model for Alkene Coordination: Zeise's Salt
The coordination of unsaturated carbon-carbon double bonds to transition metals was historically established by Zeise's salt, potassium trichloro(ethene)platinate(II) monohydrate:
The structure and bonding remained enigmatic until Michael J.S. Dewar (1951) and Joseph Chatt and L.A. Duncanson (1953) formulated the Dewar-Chatt-Duncanson (DCD) model:
Dual Bonding Components:
1. $\sigma$-Donation:
- The filled bonding $\pi$-orbital of the alkene ($\pi_{CC}$, HOMO) overlaps with an empty metal valence orbital of matching $\sigma$-symmetry (e.g., platinum $5d_{x^2-y^2}/6s/6p$ hybrid orbital):
- This interaction transfers electron density from the alkene $\pi$-bond to the metal center.
2. $\pi$-Backbonding:
- A filled metal $d$-orbital of $\pi$-symmetry ($5d_{xz}$ or $5d_{yz}$) overlaps with the empty antibonding $\pi^$ orbital of the alkene ($\pi_{CC}^$, LUMO):
- This interaction backdonates electron density from the metal into the alkene $\pi^*$ level.
Geometric Consequences in Zeise's Salt:
- In uncoordinated ethylene, the $C=C$ double bond length is $1.337$ Å, with planar $sp^2$ geometry and all four hydrogens coplanar with the carbon nuclei (dihedral angle $0^\circ$).
- In Zeise's salt, neutron diffraction reveals:
- The $C=C$ bond is oriented perpendicular to the $\text{PtCl}_3$ square plane.
- The $C-C$ bond lengthens to $1.375$ Å due to electron population of the $\pi^*$ LUMO.
- The four hydrogen atoms bend back away from the platinum atom by an angle of $\alpha \approx 32.5^\circ$, reflecting partial rehybridization of the carbon atoms from $sp^2$ toward $sp^3$.
§5.2 §5.2 The Continuum from Weak Alkene $\pi$-Complex to Metallacyclopropane
Alkene-metal bonding does not represent a static, single structural archetype; it spans a continuous spectrum between two limiting resonance extremes:
1. The Pure $\pi$-Complex Limit (Weak Backbonding):
- Prevalent for transition metals in high formal oxidation states, metals with few $d$-electrons, or late metals coordinated to electron-withdrawing coligands (e.g., $\text{Ag}(\text{I})$, $\text{Pd}(\text{II})$).
- $\sigma$-donation dominates; $\pi$-backbonding is minimal.
- The alkene retains essentially planar $sp^2$ geometry; the $C-C$ bond length is only marginally lengthened ($1.34 - 1.37$ Å).
- The metal oxidation state remains unchanged: $M^n(\eta^2-\text{alkene})$.
2. The Metallacyclopropane Limit (Extense Backbonding):
- Prevalent for electron-rich, low-valent transition metals ($d^8$ or $d^{10}$ centers like $\text{Pt}(0)$, $\text{Ni}(0)$, $\text{Fe}(0)$) or when the alkene bears strongly electron-withdrawing substituents (e.g., tetracyanoethylene TCNE, maleic anhydride).
- Metal-to-alkene $\pi$-backdonation into $\pi^*$ is so extensive that the original $C=C$ double bond order drops toward a single bond ($1.48 - 1.52$ Å).
- The two carbon atoms rehybridize completely to $sp^3$.
- Two localized, covalent $M-\text{C}$ $\sigma$-bonds form, creating a three-membered ring: a metallacyclopropane.
- The formal oxidation state of the metal center increases by $+2$ (e.g., $\text{Pt}(0) \to \text{Pt}(\text{II})$).
Quantitative Spectroscopic Indicators:
- Carbon-13 NMR: In free ethylene, $\delta(^{13}\text{C}) = 123.3\text{ ppm}$. In $\text{Pt}(\text{PPh}_3)_2(\text{C}_2\text{H}_4)$, the carbon resonance shifts upfield to $\delta = 39.6\text{ ppm}$, directly matching the $sp^3$ chemical shift regime of cyclopropane.
§5.3 §5.3 Dynamic Barriers to Alkene Rotation Around the Metal-Olefin Bond
Coordinated alkenes undergo dynamic internal rotation about the metal-alkene axis ($M-\text{centroid}$ vector). This rotation is an activated process whose barrier height directly reflects the magnitude of $\pi$-backbonding.
Orbital Mechanism of Alkene Rotation:
- Consider an alkene coordinated in the $xy$-plane of a square planar complex.
- Ground State: The $C=C$ axis lies perpendicular to the coordination plane ($z$-axis). The alkene $\pi^*$ orbital is aligned with the filled metal $d_{xz}$ orbital, maximizing $\pi$-backbonding overlap.
- Transition State: Rotating the alkene by $90^\circ$ aligns the $C=C$ axis parallel to the coordination plane.
- In this rotated orientation, the alkene $\pi^*$ orbital can no longer overlap with the $d_{xz}$ orbital.
- It must instead interact with the metal $d_{xy}$ orbital, which is often involved in in-plane $\sigma$-bonding to other ligands and lies at a lower energy level, or has inferior overlap.
- Consequently, during the $90^\circ$ rotation, $\pi$-backbonding is severely disrupted.
Quantification of Rotational Barriers:
The activation free energy $\Delta G^\ddagger_\text{rot}$ correlates directly with the metal-olefin $\pi$-backbonding strength:
- In Zeise's salt $[\text{PtCl}_3(\text{C}_2\text{H}_4)]^-$: $\Delta G^\ddagger_\text{rot} \approx 40-50\text{ kJ/mol}$ (fast rotation on the NMR timescale at room temperature).
- In electron-rich platinum(0) complexes $[\text{Pt}(\text{PPh}_3)_2(\text{C}_2\text{H}_4)]$: $\Delta G^\ddagger_\text{rot} > 85\text{ kJ/mol}$ (rotation is slow at room temperature, yielding distinct, frozen NMR signals).
- In complexes with strongly electron-withdrawing alkenes (e.g., $\text{Fe}(\text{CO})_4(\text{TCNE})$): $\Delta G^\ddagger_\text{rot} > 130\text{ kJ/mol}$ (rotation is completely locked up to decomposition).
§5.4 §5.4 Alkyne Complexes: 2-Electron vs. 4-Electron Donors & Metallacyclopropenes
Alkynes ($R-\text{C}\equiv\text{C}-R$) possess two mutually orthogonal sets of $\pi$-orbitals: $\pi_\parallel$ (parallel to the coordination plane) and $\pi_\perp$ (perpendicular to the coordination plane), along with two corresponding sets of antibonding orbitals: $\pi_\parallel^$ and $\pi_\perp^$.
Coordination Modes:
1. 2-Electron Donor ($L$-type):
- The alkyne donates its $\pi_\parallel$ bonding pair to an empty metal $\sigma$-orbital, while a filled metal $d_\pi$-orbital backdonates into $\pi_\parallel^*$.
- The orthogonal $\pi_\perp$ system remains non-bonding and unperturbed.
- Example: $[\text{Pt}(\text{PPh}_3)_2(Ph\text{C}\equiv\text{C}Ph)]$ (16e or 18e center).
2. 4-Electron Donor ($L_2$- or $LX$-type):
- In electron-deficient early transition metal or high-oxidation state complexes (e.g., $d^0 - d^2$ complexes of $\text{Mo}, \text{W}, \text{Re}$), the metal center possesses two empty valence orbitals of appropriate symmetry.
- The alkyne donates both its $\pi_\parallel$ pair and its orthogonal $\pi_\perp$ pair into the metal center:
- Example: $[\text{W}(\text{CO})(Ph\text{C}\equiv\text{C}Ph)_3]$ where each alkyne donates 4 electrons, yielding an 18-electron tungsten center ($6 + 2 + 3 \times 4 = 20$? No: W(6) + CO(2) + 2(4e alkyne) + 1(2e alkyne) = 18e!).
Bend-Back Angles and Metallacyclopropene Character:
Upon coordination, the $R-\text{C}\equiv\text{C}$ bond angles bend back from linear ($180^\circ$) to $130^\circ-145^\circ$. Extensive backdonation produces a metallacyclopropene intermediate with significant $M-\text{C}$ double bond character.
§5.5 §5.5 Synthesis and Electronic Structure of $\eta^3$-Allyl Complexes
The allyl ligand ($\text{C}_3\text{H}_5$) can coordinate in a monohapto mode ($\eta^1-\text{allyl}$, 1-electron $X$-donor) or a trihapto mode ($\eta^3-\text{allyl}$, 3-electron $LX$-donor).
Molecular Orbitals of the Free Allyl Fragment:
The three $2p_z$ orbitals of the planar trimethine chain combine into three molecular orbitals:
- $\psi_1$ (Bonding, zero nodes): $\psi_1 = \frac{1}{2} p_1 + \frac{1}{\sqrt{2}} p_2 + \frac{1}{2} p_3$ (donates to metal $s, p_z, d_{z^2}$).
- $\psi_2$ (Non-bonding, one node at C2): $\psi_2 = \frac{1}{\sqrt{2}} p_1 - \frac{1}{\sqrt{2}} p_3$ (donates to metal $p_x, d_{xz}$).
- $\psi_3$ (Antibonding, two nodes): $\psi_3 = \frac{1}{2} p_1 - \frac{1}{\sqrt{2}} p_2 + \frac{1}{2} p_3$ (accepts backdonation from metal $d_{yz}$).
Primary Synthetic Methods:
1. Oxidative Addition to Allylic Halides:
2. Nucleophilic Attack on 1,3-Dienes:
3. Deprotonation of Alkene Complexes:
§5.6 §5.6 Dynamic Fluxionality in Allyl Complexes: Syn-Anti Isomerism & Ring Slipping
Coordinated $\eta^3$-allyl ligands display dynamic stereochemical fluxionality that can be monitored by variable-temperature $^1\text{H}$ NMR spectroscopy.
Structural Non-Equivalence in Static $\eta^3$-Allyl:
In a static $\eta^3$-allyl complex ($C_s$ local symmetry):
- The central proton ($H_c$ at C2) resonates at $\delta = 4.5-5.5\text{ ppm}$ ($1\text{H}$, multiplet).
- The two terminal syn-protons ($H_s$, pointing toward the central proton) resonate at $\delta = 3.5-4.5\text{ ppm}$ ($2\text{H}$, doublet).
- The two terminal anti-protons ($H_a$, pointing away from the central proton) resonate at $\delta = 2.0-3.0\text{ ppm}$ ($2\text{H}$, doublet).
- The three environments are chemically and magnetically distinct ($1:2:2$ integration ratio).
Dynamic Exchange Mechanisms:
At elevated temperatures, the syn- and anti-resonances broaden and coalesce into a single $4\text{H}$ doublet via two primary mechanisms:
1. $\eta^3 \rightleftharpoons \eta^1 \rightleftharpoons \eta^3$ Mechanism ($\pi-\sigma-\pi$ Exchange):
- One terminal $M-\text{C}$ bond dissociates, generating a transient 16-electron $\sigma$-allyl ($\eta^1$-allyl) intermediate.
- Rapid rotation of $180^\circ$ occurs around the resulting carbon-carbon single bond ($C_\alpha-C_\beta$):
- Re-coordination into the $\eta^3$-mode exchanges the syn and anti positions.
- This process is accelerated by coordinating Lewis bases (e.g., phosphines, solvent) that stabilize the 16e $\eta^1$-intermediate.
2. Apparent Allyl Inversion via Metal Rotation:
- Rotation of the $\eta^3$-allyl ligand around the metal-centroid axis interconverts the two coordination faces.
§5.7 §5.7 Nucleophilic Attack on Coordinated $\pi$-Ligands & Davies-Green-Mingos (DGM) Rules
Coordinating an unsaturated organic ligand to a cationic or electron-deficient transition metal center withdraws electron density, inverting its chemical reactivity from nucleophilic to strongly electrophilic.
The Davies-Green-Mingos (DGM) Rules:
Steve Davies, Malcolm Green, and Michael Mingos formulated empirical stereoelectronic rules predicting the site of nucleophilic attack on polyene complexes:
1. Rule 1: Even vs. Odd Hapticity:
- Nucleophilic attack occurs preferentially at even-numbered polyenes ($\eta^2, \eta^4, \eta^6$) rather than odd-numbered polyenes ($\eta^3, \eta^5, \eta^7$):
- Example: In $[(\eta^5-\text{Cp})(\eta^6-\text{benzene})\text{Fe}]^+$, attack occurs exclusively on the even $\eta^6$-benzene ring, yielding an $(\eta^5-\text{cyclohexadienyl})$ complex.
2. Rule 2: Open vs. Closed Polyenes:
- For ligands of the same hapticity, nucleophilic attack occurs preferentially at open (acyclic) polyenes rather than closed (cyclic) polyenes:
- Example: In an 18e complex containing an open $\eta^5$-pentadienyl and a closed $\eta^5$-cyclopentadienyl, attack occurs exclusively at the open pentadienyl ligand.
3. Rule 3: Terminal vs. Internal Attack:
- For even, open polyenes, attack occurs at the terminal carbon atom:
- For odd, open polyenes, attack occurs at the terminal carbon only if the metal complex is strongly electron-withdrawing; otherwise, internal attack is observed.
§5.8 §5.8 The Tsuji-Trost Allylic Alkylation: Mechanism and Stereocontrol
The Tsuji-Trost reaction is a premier carbon-carbon bond forming reaction in organic synthesis, involving palladium-catalyzed substitution of allylic esters, carbonates, or halides by soft nucleophiles:
Catalytic Cycle and Stereochemical Trajectory:
1. $\eta^2$-Olefin Coordination: The palladium(0) catalyst $L_2\text{Pd}(0)$ coordinates the allylic double bond.
2. Ionization (Oxidative Addition):
- Palladium attacks the allylic system from the face opposite to the leaving group (inversion of configuration at carbon).
- Departure of the leaving group ($-\text{OAc}^-$) yields a cationic $[(\eta^3-\text{allyl})\text{Pd}L_2]^+$ intermediate.
3. Nucleophilic Attack:
- Soft Nucleophiles ($\text{p}K_a < 25$, e.g., malonates, amines, $\beta$-ketoesters):
Attack occurs directly at the allyl carbon from the face opposite to palladium (anti-attack, outer-sphere mechanism). This incurs a second inversion of configuration.
- Overall Stereochemical Outcome: Retention of Configuration (Inversion $+$ Inversion $=$ Net Retention).
- Hard Nucleophiles (e.g., organolithiums, Grignard reagents):
Attack occurs first directly at the palladium center (transmetallation, inner-sphere mechanism), followed by reductive elimination onto the allyl ligand.
- Overall Stereochemical Outcome: Net Inversion of Configuration (Inversion $+$ Retention $=$ Net Inversion).
Enantioselective Tsuji-Trost alkylations employ chiral diphosphine ligands (e.g., the Trost ligand), achieving $>99\%$ enantiomeric excess.
Worked Practice Problems (9 Challenge Exercises)
Multi-step solved problems covering neutral vs ionic electron counting, d-electron configuration determination, 16-electron square planar stabilization, metal-metal single and multiple bond orders, bridging ligand electron partitioning, and 3c-2e bridge thermodynamic equilibria with line-by-line mathematical proofs.
In Zeise's salt $\text{K}[\text{PtCl}_3(\eta^2-\text{C}_2\text{H}_4)]\cdot\text{H}_2\text{O}$: (a) Calculate the formal oxidation state, $d$-electron count, and total valence electron count ($VEC$) of platinum. (b) Explain why the ethylene ligand coordinates with its $C=C$ axis perpendicular to the $\text{PtCl}_3$ square plane. (c) Account for the observed bending back of the four hydrogens ($\alpha = 32.5^\circ$) using hybridization changes.
Line-by-Line Solution:
(a) Formal Oxidation State and Electron Count:
- Ligand charges: Three chloride ligands ($-1$ each) and one neutral ethylene ligand ($L$, formal charge $0$).
- The complex anion is $[\text{PtCl}_3(\text{C}_2\text{H}_4)]^-$ with net charge $q = -1$.
- Platinum is in Group 10 ($n_v = 10$):
- Total valence electron count ($VEC$):
- $\text{Pt}(\text{II})$: 8 electrons
- Three $\text{Cl}^-$: $3 \times 2 = 6$ electrons
- One $\eta^2-\text{C}_2\text{H}_4$: 2 electrons
- A classic 16-electron square planar $d^8$ transition metal complex.
(b) Orientation of the $C=C$ Axis Perpendicular to the Square Plane:
- In a square planar $d^8$ complex in the $xy$-plane, the empty metal orbital accepting the $\sigma$-dative pair from the alkene $\pi$-orbital is a $5d/6s/6p$ hybrid pointing along an in-plane coordination vector (say, along the $x$-axis).
- For $\pi$-backbonding, the metal must utilize a filled $d$-orbital directed toward the alkene $\pi^*$ LUMO.
- If the $C=C$ bond lies in the $xy$-plane (parallel):
- The metal orbital of matching $\pi$-symmetry would have to be $d_{xy}$.
- However, $d_{xy}$ is directed between the four in-plane ligands, experiencing strong steric and electrostatic repulsion with the cis chlorides.
- If the $C=C$ bond is oriented perpendicular to the plane (along the $z$-axis):
- The alkene $\pi^*$ LUMO lies in the $xz$-plane.
- It overlaps with the filled metal $5d_{xz}$ orbital, which projects above and below the coordination plane into empty space.
- This orientation provides maximum orbital overlap for $\pi$-backbonding and minimizes steric clash with the adjacent cis chloride ligands.
(c) Bending Back of the Hydrogen Atoms:
- In uncoordinated ethylene, the carbons are $sp^2$ hybridized with $120^\circ$ planar geometry.
- As metal-to-ligand $\pi$-backdonation populates the $\pi^*$ LUMO, electron density between the two carbon nuclei drops, while electron density in the $Pt-C$ bonding region increases.
- The carbon atoms rehybridize from $sp^2$ toward $sp^3$.
- To attain tetrahedral-like geometry around each carbon atom, the four hydrogen substituents bend away from the platinum atom.
- In Zeise's salt, the observed dihedral bend-back angle is $\alpha = 32.5^\circ$, corresponding to intermediate character between planar ethylene ($0^\circ$) and fully $sp^3$ metallacyclopropane ($109.5^\circ - 90^\circ \approx 54^\circ$).
An allyl complex of formula $[\text{Pd}(\text{C}_3\text{H}_5)(\text{PPh}_3)\text{Cl}]$ exists as two distinct coordination isomers. (a) State the hapticity and electron count of the allyl ligand in the $\eta^1$-mode versus the $\eta^3$-mode. (b) Predict the number of $^1\text{H}$ NMR signals and their relative intensities for both isomers in a low-temperature static limit. (c) State which isomer is thermodynamically preferred for palladium(II).
Line-by-Line Solution:
(a) Hapticity and Electron Counting:
- $\eta^1-\text{Allyl}$ (monohapto):
- Bound through a single $M-\text{C}$ $\sigma$-bond.
- Acts as a 1-electron donor in the neutral model ($X$-type) or 2-electron donor as allyl anion ($ ext{C}_3 ext{H}_5^-$).
- The remaining two carbons form an uncoordinated pendant $C=C$ double bond.
- $\eta^3-\text{Allyl}$ (trihapto):
- Bound through all three contiguous carbon atoms.
- Acts as a 3-electron donor in the neutral model ($LX$-type) or 4-electron donor as allyl anion.
(b) Low-Temperature Static $^1\text{H}$ NMR Spectral Prediction:
1. For the $\eta^1-\text{Allyl}$ Isomer ($M-\text{CH}_2-\text{CH}=\text{CH}_2$):
- Contains a localized $\sigma$-alkyl methylene group and a vinyl group.
- Shows three sets of protons:
- Methylene protons ($-\text{CH}_2-M$): $2\text{H}$ at $\delta \approx 2.0-2.5\text{ ppm}$
- Internal vinyl proton ($-\text{CH}=$): $1\text{H}$ at $\delta \approx 5.8-6.2\text{ ppm}$
- Terminal vinyl protons ($=\text{CH}_2$): $2\text{H}$ (split into cis/trans) at $\delta \approx 4.8-5.2\text{ ppm}$
- Total: 3 distinct signals (or 4 if terminal vinyl protons are diastereotopic) with integration ratio $2 : 1 : 2$.
2. For the $\eta^3-\text{Allyl}$ Isomer:
- Exhibits $C_s$ mirror plane symmetry passing through the central carbon and the metal atom.
- Shows three distinct signals:
- Central proton ($H_c$ at C2): $1\text{H}$ multiplet at $\delta \approx 4.8-5.5\text{ ppm}$
- Two syn-protons ($H_s$ at C1, C3): $2\text{H}$ doublet at $\delta \approx 3.8-4.2\text{ ppm}$
- Two anti-protons ($H_a$ at C1, C3): $2\text{H}$ doublet at $\delta \approx 2.8-3.2\text{ ppm}$
- Total: Exactly 3 signals with integration ratio $1 : 2 : 2$.
(c) Thermodynamic Preference for $\text{Pd}(\text{II})$:
- In $[\text{Pd}(\eta^1-\text{C}_3\text{H}_5)(\text{PPh}_3)\text{Cl}]$, palladium is 3-coordinate and possesses only:
- In $[\text{Pd}(\eta^3-\text{C}_3\text{H}_5)(\text{PPh}_3)\text{Cl}]$, the $\eta^3$-allyl donates 4 electrons (ionic model):
- 16 valence electrons represents the closed-shell, thermodynamically stable configuration for square planar $d^8$ $\text{Pd}(\text{II})$.
- Therefore, the $\eta^3-\text{allyl}$ isomer is overwhelmingly favored thermodynamically by $>60\text{ kJ/mol}$.
Predict the exact site of nucleophilic attack by methoxide ($\text{MeO}^-$) on the following cationic complexes using the Davies-Green-Mingos rules: (a) $[(\eta^5-\text{C}_5\text{H}_5)(\eta^6-\text{C}_6\text{H}_6)\text{Fe}]^+$, (b) $[(\eta^5-\text{C}_5\text{H}_5)(\eta^4-\text{C}_4\text{H}_6)\text{Fe}(\text{CO})]^+$, (c) $[(\eta^5-\text{C}_5\text{H}_5)\text{Mo}(\text{CO})_2(\eta^3-\text{C}_3\text{H}_5)]^+$.
Line-by-Line Solution:
(a) $[(\eta^5-\text{C}_5\text{H}_5)(\eta^6-\text{C}_6\text{H}_6)\text{Fe}]^+$:
- Ligands present: $\eta^5-\text{cyclopentadienyl}$ (odd, closed) and $\eta^6-\text{benzene}$ (even, closed).
- Apply Rule 1: Nucleophiles attack even polyenes preferentially over odd polyenes:
- Attack occurs exclusively on the $\eta^6-\text{benzene}$ ring, converting it into an uncharged neutral $\eta^5-\text{cyclohexadienyl}$ complex:
(b) $[(\eta^5-\text{C}_5\text{H}_5)(\eta^4-\text{C}_4\text{H}_6)\text{Fe}(\text{CO})]^+$:
- Ligands present: $\eta^5-\text{Cp}$ (odd, closed) and $\eta^4-\text{butadiene}$ (even, open).
- Apply Rule 1: Attack occurs at the even polyene ($\eta^4-\text{butadiene}$) rather than the odd polyene ($\eta^5-\text{Cp}$).
- Apply Rule 3: For even, open polyenes, attack occurs preferentially at the terminal carbon (C1 or C4):
- Attack delivers a neutral $\eta^3-\text{allyl}$ complex: $(\eta^5-\text{Cp})\text{Fe}(\text{CO})(\eta^3-\text{CH}_2\text{CHCHCH}_2\text{OMe})$.
(c) $[(\eta^5-\text{C}_5\text{H}_5)\text{Mo}(\text{CO})_2(\eta^3-\text{C}_3\text{H}_5)]^+$:
- Both polyene ligands are odd: $\eta^5-\text{Cp}$ (odd, closed) and $\eta^3-\text{allyl}$ (odd, open).
- Apply Rule 2: Between ligands of comparable parity, attack occurs at the open polyene rather than the closed polyene:
- Apply Rule 3: Attack occurs at a terminal carbon of the allyl ligand, generating a neutral $\eta^2-\text{alkene}$ complex:
The square planar complex $[\text{PtCl}_2(\text{PEt}_3)(\eta^2-\text{C}_2\text{Me}_4)]$ possesses a coordinated tetramethylethylene ligand. At $-50^\circ\text{C}$, the four methyl groups appear as two distinct $^1\text{H}$ singlets separated by $\Delta \nu = 48\text{ Hz}$ due to frozen rotation. At coalescence temperature $T_c = +10^\circ\text{C}$, the two peaks merge into a single broad singlet. (a) Calculate the rate constant of alkene rotation $k_c$ at coalescence. (b) Calculate the activation enthalpy $\Delta H^\ddagger$ and activation entropy $\Delta S^\ddagger$ if $\Delta G^\ddagger = 61.2\text{ kJ/mol}$ at $T_c$ and the rate at $-20^\circ\text{C}$ is $k = 18\text{ s}^{-1}$.
Line-by-Line Solution:
(a) Rate Constant at Coalescence ($k_c$): For an uncoupled two-site exchange with equal population probabilities:
Given $\Delta \nu = 48\text{ Hz}$:
(b) Eyring Activation Parameters ($\Delta H^\ddagger$ and $\Delta S^\ddagger$): Given:
- $T_1 = -20^\circ\text{C} = 253.15\text{ K}$, with $k_1 = 18\text{ s}^{-1}$.
- $T_c = +10^\circ\text{C} = 283.15\text{ K}$, with $k_c = 106.6\text{ s}^{-1}$.
From the linear Eyring formulation:
Let $Y = \ln(k/T)$ and $X = 1/T$:
- At $T_1 = 253.15\text{ K}$:
- At $T_c = 283.15\text{ K}$:
- Compute Slope:
- Compute Activation Enthalpy:
- Compute Activation Entropy:
From $\Delta G^\ddagger = \Delta H^\ddagger - T\Delta S^\ddagger$ at $T_c = 283.15\text{ K}$:
- Physical Interpretation: The negative activation entropy ($\Delta S^\ddagger \approx -99\text{ J/(mol}\cdot\text{K)}$) indicates an ordered transition state where solvent and ancillary phosphine ethyl groups become restricted during the $90^\circ$ rotation.
An enantiomerically pure allylic acetate $(R,E)$-1,3-diphenylallyl acetate is treated with dimethyl sodiomalonate in the presence of $1\text{ mol}\%$ $[(\eta^3-\text{C}_3\text{H}_5)\text{PdCl}]_2$ and $(R,R)$-chiraphos. (a) Trace the stereochemical configuration of the palladium-allyl intermediate. (b) Predict the absolute stereochemistry of the alkylated product. (c) Explain why using a hard alkyl Grignard reagent ($Me\text{MgBr}$) yields the inverted enantiomer.
Line-by-Line Solution:
(a) Stereochemistry of the Palladium-Allyl Intermediate:
- Starting material: $(R,E)$-1,3-diphenylallyl acetate. The acetate leaving group ($-\text{OAc}$) resides on one defined face of the allylic plane.
- In the oxidative addition step, the palladium(0) catalyst coordinates the double bond and performs a nucleophilic displacement on the acetate-bearing carbon.
- This displacement occurs via an outer-sphere inversion pathway: palladium attacks from the face opposite to the leaving acetate group:
- The resulting cationic $[(\eta^3-\text{1,3-diphenylallyl})\text{Pd}(\text{chiraphos})]^+]$ intermediate has the palladium atom located exclusively on the face opposite to the original acetate.
(b) Absolute Stereochemistry with Soft Nucleophile (Dimethyl Malonate):
- Dimethyl sodiomalonate is a stabilized carbanion ($\text{p}K_a \approx 13$, soft nucleophile).
- Soft nucleophiles attack coordinated $\eta^3$-allyl ligands via an outer-sphere mechanism:
- The malonate anion attacks the allylic carbon directly from the solution side, on the face opposite to the palladium atom.
- This nucleophilic addition proceeds with inversion of configuration at carbon:
3. Summing the two elementary steps:
- The product retains the original $(R)$ absolute configuration: $(R,E)$-dimethyl 2-(1,3-diphenylallyl)malonate.
(c) Stereochemical Divergence with Hard Nucleophile ($Me\text{MgBr}$):
- Methylmagnesium bromide is a hard, localized carbanion.
- Hard nucleophiles cannot perform outer-sphere attack on the external face of the allyl ligand.
- Instead, $Me\text{MgBr}$ attacks the electropositive palladium metal center directly via transmetallation:
- The methyl group then undergoes intramolecular reductive elimination onto the allyl carbon from the same face as the palladium atom (retention in the elimination step).
- Net Stereochemical Trajectory with Hard Nucleophile:
- Thus, the reaction with $Me\text{MgBr}$ yields the opposite $(S)$ enantiomer!
The tungsten complex $[\text{W}(\text{CO})(\text{S}_2\text{CNEt}_2)_2(\text{RC}\equiv\text{CR})]$ is diamagnetic and stable. (a) Determine the formal oxidation state of tungsten assuming the alkyne acts as a 2-electron donor vs a 4-electron donor. (b) Calculate the total valence electron count ($VEC$) for both models, and prove which donor mode satisfies the 18-electron rule. (c) Predict the effect on the $^{13}\text{C}$ NMR chemical shift of the alkyne carbons.
Line-by-Line Solution:
(a) Ligand Classifications and Oxidation States:
- $\text{CO}$ is a neutral 2-electron $L$-ligand (formal charge $0$).
- Diethyldithiocarbamate $\text{S}_2\text{CNEt}_2^-$ is a bidentate monoanionic ligand ($L X$-type, donating 4 electrons per ligand, charge $-1$).
- Two dithiocarbamate ligands carry a total charge of $-2$.
- Overall complex charge $q = 0$.
- Tungsten is in Group 6 ($n_v = 6$).
- Model 1: Alkyne as 2-Electron Donor ($L$-type, charge $0$):
- Model 2: Alkyne as 4-Electron Donor ($L_2$-type or $C^2-$ metallacyclopropene, charge $0$ or $-2$):
- Under covalent CBC model: alkyne is $L_2$, formal charge is $0$. Metal oxidation state remains $+2$ ($d^4$).
(b) Total Valence Electron Count ($VEC$):
- Under the 2-Electron Donor Hypothesis:
- Tungsten (Group 6): 6 electrons
- CO: 2 electrons
- Two dithiocarbamates: $2 \times 3\text{e}$ (neutral model: $S^\bullet + S: = 3\text{e}$ each) $= 6$ electrons
- Alkyne (2e): 2 electrons
Under this model, the tungsten center is sub-18e (16 electrons), leaving an empty valence orbital.
- Under the 4-Electron Donor Hypothesis:
- Both orthogonal $\pi$-systems ($\pi_\parallel$ and $\pi_\perp$) donate into tungsten:
- Conclusion: To achieve electronic saturation and satisfy the 18-electron rule, the alkyne must act as a 4-electron donor ($L_2$).
(c) $^{13}\text{C}$ NMR Chemical Shift Prediction:
- For free alkynes, $sp$-hybridized carbons resonate at $\delta = 70 - 90\text{ ppm}$.
- In a 2-electron alkyne complex, carbons shift downfield to $\delta = 110 - 150\text{ ppm}$.
- In a 4-electron donor alkyne complex, both $\pi$-orbitals donate heavily into the metal, while the metal backdonates into $\pi^*$. The $C-C$ bond order approaches a single bond, and the carbons experience extreme downfield deshielding:
This downfield shift (in the range typical of carbenes and metal-alkylidynes) is the definitive spectroscopic signature of a 4-electron donating alkyne.
Prove Rule 1 of the Davies-Green-Mingos theory using perturbation molecular orbital theory. Show mathematically why an incoming nucleophile interacts more favorably with the LUMO of an even polyene complex $[M(\eta^{2n}-\text{C}_{2n}\text{H}_{2n})]^{+m}$ than an odd polyene complex $[M(\eta^{2n+1}-\text{C}_{2n+1}\text{H}_{2n+1})]^{+m}$.
Line-by-Line Solution:
1. Perturbation Energy for Nucleophilic Attack: According to Klopman-Salem frontier molecular orbital theory, the stabilization energy $\Delta E$ upon interaction between a nucleophile ($ ext{Nu}$) and a coordinated polyene complex is:
where the second term represents the frontier orbital charge-transfer interaction.
2. Frontier Orbital Energy of Coordinated Polyenes: Consider the Hückel $\pi$-orbital levels of even ($2n$) versus odd ($2n+1$) polyenes:
- Even Closed Polyenes (e.g., Benzene, $2n = 6$):
- Ground-state neutral benzene has 6 electrons completely filling the three bonding MOs ($a_{1g}, e_{1g}$).
- Coordination to a transition metal in an 18-electron complex involves donation from $a_{1g}$ and $e_{1g}$ into empty metal orbitals, and backdonation from metal $d$ into the degenerate $e_{2u}$ LUMO.
- However, because the complex bears a formal positive charge ($+m$), the entire orbital manifold is depressed to low energy.
- The lowest unoccupied molecular orbital (LUMO) of the complex has substantial amplitude localized on the ligand carbon atoms with a low orbital energy $E_\text{LUMO}$, producing a small denominator $E_\text{LUMO} - E_\text{HOMO}(\text{Nu})$ and a large orbital interaction $\Delta E$.
- Odd Polyenes (e.g., Cyclopentadienyl $Cp$, $2n+1 = 5$):
- The cyclopentadienyl ligand is formally a $6\pi$ aromatic system as $Cp^-$ ($e_{1g}$ completely filled).
- Its LUMO is $e_{2u}^*$, which lies at an exceptionally high energy level ($> +3\text{ eV}$ higher than benzene $e_{2u}$).
- Even upon coordination to a cationic metal center, the $Cp$ $e_{2u}^*$ orbital remains at a prohibitive energy level.
- Instead, the LUMO of the complex is primarily metal-centered ($d_{z^2}^$ or $e_g^$), with negligible atomic orbital coefficients $c_i$ on the cyclopentadienyl carbon atoms ($c_i \approx 0$).
3. Comparison of Atomic Orbital Coefficients ($c_i$):
- In even polyene complexes ($\eta^6-\text{benzene}$, $\eta^4-\text{diene}$), the LUMO has large coefficients at the carbon atoms ($|c_i| \approx 0.4 - 0.6$).
- In odd polyene complexes ($\eta^5-\text{Cp}$), the LUMO is metal-localized ($c_\text{carbon} \approx 0.05$).
- Consequently:
- Therefore, nucleophilic attack on even polyenes is favored both electrostatically and by frontier orbital overlap by factors exceeding $10^5$, establishing the theoretical foundation of DGM Rule 1.
The dynamic exchange of syn and anti protons in $[(\eta^3-\text{C}_3\text{H}_5)\text{Pd}(\text{PR}_3)\text{Cl}]$ follows the $\pi-\sigma-\pi$ pathway. (a) Derive the steady-state kinetic expression for the exchange rate $k_\text{obs}$ in the presence of an added Lewis base $L$. (b) Explain why the reaction is first-order in $[L]$ at low base concentration and approaches zero-order saturation at high $[L]$. (c) Construct the orbital correlation diagram connecting $\eta^3-\text{allyl}$ to the 16e $\eta^1-\text{allyl}$ intermediate.
Line-by-Line Solution:
(a) Kinetic Derivation of $\pi-\sigma-\pi$ Exchange with Added Base $L$:
- Let the starting 16-electron complex be $\text{Pd}_{\eta^3}$.
- Step 1: Associative Attack of Base $L$:
Incoming base $L$ coordinates to palladium, inducing an $\eta^3 \to \eta^1$ hapticity ring slip:
3. Step 2: Carbon-Carbon Single Bond Rotation:
In the 16-electron $\sigma$-allyl intermediate, rotation around the $C_\alpha-C_\beta$ bond occurs with rate constant $k_\text{rot}$:
4. Step 3: Dissociation of $L$ and Re-coordination:
Applying the steady-state approximation to the intermediate $[\text{Pd}_{\eta^1}-L]$:
The observed rate of exchange of syn/anti protons is:
Thus, the apparent pseudo-first-order rate constant is:
(b) Saturation Kinetic Regimes:
1. At Low Base Concentration or Fast Rotation ($k_{-1} \gg k_\text{rot}$):
The exchange rate depends linearly on $[L]$ (first-order kinetics).
2. At High Base Concentration ($k_\text{rot} \gg k_{-1}$ or rapid pre-equilibrium):
When coordination of $L$ is quantitative, the rate-determining step becomes the intrinsic single-bond rotation $k_\text{rot}$:
The exchange rate becomes independent of $[L]$ (zero-order saturation).
(c) Orbital Correlation Diagram ($\eta^3 \to \eta^1$):
- In $\eta^3-\text{allyl}$, the three carbon $p$-orbitals form $\psi_1, \psi_2, \psi_3$. Both $\psi_1$ (symmetric) and $\psi_2$ (antisymmetric) overlap with metal $d$-orbitals, donating 4 electrons.
- As one terminal carbon $C_3$ pulls away:
- $\psi_1$ and $\psi_2$ re-hybridize into a localized $C_1-M$ $\sigma$-bonding orbital and a localized $C_2=C_3$ $\pi$-bonding orbital.
- The metal $d$-orbital previously bonded to $C_3$ becomes vacant, receiving the electron pair from the incoming base $L$.
- The $C_1-C_2$ bond becomes a pure $\sigma$-single bond, allowing barrier-free rotation ($E_a \approx 25-35\text{ kJ/mol}$) before reverse slip regenerates $\eta^3$ with exchanged proton environments.
In the Tsuji-Trost allylic alkylation of an unsymmetrical substrate $[(\eta^3-\text{1-methylallyl})\text{Pd}(P-P)]^+$, attack by dimethyl malonate can occur at C1 (branched product) or C3 (linear product). (a) Explain why steric effects favor attack at C3, whereas electronic ground-state trans-influence favors attack at C1. (b) For an unsymmetrical bidentate ligand where $P_1$ is a strong $\sigma$-donor (alkylphosphine) and $P_2$ is a strong $\pi$-acceptor (phosphite), predict the major regioisomer. (c) Derive the mathematical relation between the enantiomeric excess ($ee$) and the difference in transition-state activation free energies $\Delta\Delta G^\ddagger$.
Line-by-Line Solution:
(a) Steric vs. Electronic Regiocontrol:
1. Steric Factor:
- C1 bears a methyl substituent; C3 bears only hydrogen atoms.
- Bulky nucleophiles or sterically encumbered diphosphine ligands favor attack at the less hindered, unsubstituted terminus C3, yielding the linear product ($E$-alkene).
2. Electronic Ground-State Trans-Influence:
- The methyl group at C1 is an electron-releasing inductive substituent ($+I$), which stabilizes the partial positive charge developing in the transition state.
- Furthermore, according to the trans-influence, the carbon terminus trans to the stronger trans-influence ligand experiences greater $Pd-C$ bond lengthening and higher carbocationic character, directing nucleophilic attack to that site.
(b) Regiochemical Outcome with Unsymmetrical $P_1-P_2$ Ligand:
- $P_1$ is a strong $\sigma$-donor (e.g., $\text{PMe}_3$, alkylphosphine).
- $P_2$ is a strong $\pi$-acceptor (e.g., $\text{P(OPh)}_3$, phosphite).
- In square planar $[(\eta^3-\text{allyl})\text{Pd}(P_1)(P_2)]^+$, one allyl terminus is trans to $P_1$, and the other is trans to $P_2$.
- The strong $\sigma$-donor $P_1$ exerts a large trans-influence: it directs electron density into the metal, weakening and lengthening the trans $Pd-\text{C}$ bond.
- However, the strong $\pi$-acceptor $P_2$ withdraws electron density from the metal. The allyl carbon trans to $P_2$ receives significantly less backdonation, rendering it more electrophilic (more carbocationic).
- Nucleophilic attack by soft carbanions (dimethyl malonate) occurs preferentially at the allyl terminus trans to the stronger $\pi$-acceptor ($P_2$).
- By designing ligands where the more sterically accessible or substituted carbon aligns trans to the $\pi$-acceptor, the reaction can be steered selectively toward either the linear or branched product with $>95:5$ regiocontrol.
(c) Mathematical Derivation of Enantiomeric Excess ($ee$): In an asymmetric catalytic reaction where two enantiomeric pathways proceed through transition states $TS_R$ and $TS_S$ with activation free energies $\Delta G_R^\ddagger$ and $\Delta G_S^\ddagger$:
- According to transition-state theory:
- The enantiomeric ratio ($er$) is:
where $\Delta\Delta G^\ddagger = \Delta G_S^\ddagger - \Delta G_R^\ddagger > 0$ (assuming $R$ is favored).
- The enantiomeric excess ($ee$) is defined as:
- Substituting $er = \exp\left(\frac{\Delta\Delta G^\ddagger}{RT}\right)$:
- Numerical Benchmark at $298\text{ K}$:
- For $90\%\ ee$: $er = 19:1 \implies \Delta\Delta G^\ddagger = RT \ln(19) = (8.314)(298)(2.944) = 7.3\text{ kJ/mol}$ ($1.74\text{ kcal/mol}$).
- For $99\%\ ee$: $er = 199:1 \implies \Delta\Delta G^\ddagger = RT \ln(199) = 13.1\text{ kJ/mol}$ ($3.13\text{ kcal/mol}$).
A difference of just $3\text{ kcal/mol}$ in transition state free energy delivers near-perfect enantioselectivity!