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Chapter 5 • Theory & Derivations

pi-Complexes I: Alkenes, Alkynes & eta3-Allyl Complexes

Dewar-Chatt-Duncanson bonding model for alkene coordination, Zeise's salt, metallacyclopropanes, dynamic rotational barriers around metal-olefin bonds, 2-electron vs 4-electron alkyne donors, synthesis and electronic structure of eta3-allyl complexes, dynamic fluxionality and syn-anti exchange mechanisms, Davies-Green-Mingos (DGM) rules, and the Tsuji-Trost asymmetric allylic alkylation.

§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:

\[\text{K}[\text{PtCl}_3(\eta^2-\text{C}_2\text{H}_4)]\cdot\text{H}_2\text{O}\]

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):
\[M \xleftarrow{\quad\sigma\quad} (\eta^2-\text{C}=\text{C})\]
  • 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):
\[d_\pi(M) \xrightarrow{\quad\pi\quad} \pi_{CC}^*\]
  • 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:
\[M \xleftarrow{\quad\sigma_1\quad} \pi_\parallel \quad \text{and} \quad M \xleftarrow{\quad\sigma_2\quad} \pi_\perp\]
  • 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:

  1. $\psi_1$ (Bonding, zero nodes): $\psi_1 = \frac{1}{2} p_1 + \frac{1}{\sqrt{2}} p_2 + \frac{1}{2} p_3$ (donates to metal $s, p_z, d_{z^2}$).
  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 $p_x, d_{xz}$).
  3. $\psi_3$ (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:

\[\text{Ni}(\text{CO})_4 + \text{H}_2\text{C}=\text{CH}-\text{CH}_2\text{Cl} \longrightarrow \frac{1}{2}\,[(\eta^3-\text{C}_3\text{H}_5)\text{Ni}(\mu-\text{Cl})]_2 + 4\,\text{CO} \uparrow\]
\[\text{PdCl}_2 + \text{allyl alcohol} \xrightarrow{\text{CO, MeOH}} [(\eta^3-\text{C}_3\text{H}_5)\text{Pd}(\mu-\text{Cl})]_2\]

2. Nucleophilic Attack on 1,3-Dienes:

\[[(\eta^4-\text{butadiene})\text{Co}(\text{CO})_3]^+ + \text{H}^- \longrightarrow (\eta^3-\text{crotyl})\text{Co}(\text{CO})_3\]

3. Deprotonation of Alkene Complexes:

\[[L_n M(\eta^2-\text{propene})]^+ + \text{Base} \longrightarrow L_n M(\eta^3-\text{allyl}) + \text{H-Base}^+\]

§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 ($C_\alpha-C_\beta$):
\[\eta^3-\text{allyl} \xrightleftharpoons[k_{-1}]{k_1} [\eta^1-\text{allyl}] \xrightarrow{\text{rotation}} [\eta^1-\text{allyl}]' \xrightleftharpoons[k_1]{k_{-1}} (\eta^3-\text{allyl})'\]
  • 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 ($\eta^3, \eta^5, \eta^7$):
\[\text{Even } (\eta^{2n}) > \text{Odd } (\eta^{2n+1})\]
  • 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:
\[\text{Open polyenes} > \text{Closed polyenes}\]
  • 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:
\[\text{Terminal position} > \text{Internal position}\]
  • 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:

\[\text{R-CH}=\text{CH}-\text{CH}_2\text{OAc} + \text{Nu}^- \xrightarrow{\text{Pd(0) cat.},\, L_2} \text{R-CH(Nu)}-\text{CH}=\text{CH}_2 + \text{AcO}^-\]

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.

Foundational Example 5.1: Structural and Geometric Analysis of Zeise's Salt

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:

  1. Ligand charges: Three chloride ligands ($-1$ each) and one neutral ethylene ligand ($L$, formal charge $0$).
  2. The complex anion is $[\text{PtCl}_3(\text{C}_2\text{H}_4)]^-$ with net charge $q = -1$.
\[OS(\text{Pt}) = -1 - [3(-1) + 0] = -1 - (-3) = +2 \implies \text{Pt}(\text{II})\]
  1. Platinum is in Group 10 ($n_v = 10$):
\[d^n = n_v - OS = 10 - 2 = 8 \implies d^8\]
  1. 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
\[VEC = 8 + 6 + 2 = 16\text{ electrons}\]
  • A classic 16-electron square planar $d^8$ transition metal complex.

(b) Orientation of the $C=C$ Axis Perpendicular to the Square Plane:

  1. 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).
  2. For $\pi$-backbonding, the metal must utilize a filled $d$-orbital directed toward the alkene $\pi^*$ LUMO.
  3. 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.
  1. 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:

  1. In uncoordinated ethylene, the carbons are $sp^2$ hybridized with $120^\circ$ planar geometry.
  2. 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.
  3. The carbon atoms rehybridize from $sp^2$ toward $sp^3$.
  4. To attain tetrahedral-like geometry around each carbon atom, the four hydrogen substituents bend away from the platinum atom.
  5. 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 ($109.5^\circ - 90^\circ \approx 54^\circ$).
Foundational Example 5.2: NMR Distinction and Coordination Modes of Allyl Ligands

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:
\[VEC = 8 (\text{Pd}^{II}) + 2 (\text{Cl}^-) + 2 (\text{PPh}_3) + 2 (\eta^1-\text{allyl}) = 14\text{ valence electrons}\]
  • 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):
\[VEC = 8 + 2 + 2 + 4 = 16\text{ valence electrons}\]
  • 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 $>60\text{ kJ/mol}$.
Foundational Example 5.3: Application of the Davies-Green-Mingos (DGM) Rules

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:
\[\text{Even } (\eta^6) > \text{Odd } (\eta^5)\]
  • Attack occurs exclusively on the $\eta^6-\text{benzene}$ ring, converting it into an uncharged neutral $\eta^5-\text{cyclohexadienyl}$ complex:
\[[(\eta^5-\text{Cp})(\eta^6-\text{C}_6\text{H}_6)\text{Fe}]^+ + \text{MeO}^- \longrightarrow (\eta^5-\text{Cp})(\eta^5-\text{C}_6\text{H}_6\text{OMe})\text{Fe}\]

(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):
\[\text{Terminal position } (C1) > \text{Internal position } (C2)\]
  • 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:
\[\text{Open } (\eta^3-\text{allyl}) > \text{Closed } (\eta^5-\text{Cp})\]
  • Apply Rule 3: Attack occurs at a terminal carbon of the allyl ligand, generating a neutral $\eta^2-\text{alkene}$ complex:
\[(\eta^5-\text{Cp})\text{Mo}(\text{CO})_2(\eta^2-\text{H}_2\text{C}=\text{CH}-\text{CH}_2\text{OMe})\]
Intermediate Example 5.4: Variable-Temperature NMR Kinetics of Alkene Rotation

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:

\[k_c = \frac{\pi \Delta \nu}{\sqrt{2}}\]

Given $\Delta \nu = 48\text{ Hz}$:

\[k_c = \frac{3.14159 \times 48}{1.4142} = \frac{150.80}{1.4142} \approx 106.6\text{ s}^{-1}\]

(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:

\[\ln\left(\frac{k}{T}\right) = \ln\left(\frac{k_B}{h}\right) + \frac{\Delta S^\ddagger}{R} - \frac{\Delta H^\ddagger}{R T}\]

Let $Y = \ln(k/T)$ and $X = 1/T$:

  • At $T_1 = 253.15\text{ K}$:
\[X_1 = \frac{1}{253.15} = 3.9502 \times 10^{-3}\text{ K}^{-1}\]
\[Y_1 = \ln\left(\frac{18}{253.15}\right) = \ln(0.07110) = -2.6436\]
  • At $T_c = 283.15\text{ K}$:
\[X_2 = \frac{1}{283.15} = 3.5317 \times 10^{-3}\text{ K}^{-1}\]
\[Y_2 = \ln\left(\frac{106.6}{283.15}\right) = \ln(0.37648) = -0.9769\]
  1. Compute Slope:
\[\text{Slope} = \frac{Y_2 - Y_1}{X_2 - X_1} = \frac{-0.9769 - (-2.6436)}{(3.5317 - 3.9502) \times 10^{-3}} = \frac{+1.6667}{-0.4185 \times 10^{-3}} = -3982.6\text{ K}\]
  1. Compute Activation Enthalpy:
\[-\frac{\Delta H^\ddagger}{R} = \text{Slope} \implies \Delta H^\ddagger = -R \times \text{Slope}\]
\[\Delta H^\ddagger = -(8.3145\text{ J/(mol}\cdot\text{K)})(-3982.6\text{ K}) = +33,113\text{ J/mol} \approx 33.1\text{ kJ/mol}\]
  1. Compute Activation Entropy:

From $\Delta G^\ddagger = \Delta H^\ddagger - T\Delta S^\ddagger$ at $T_c = 283.15\text{ K}$:

\[\Delta S^\ddagger = \frac{\Delta H^\ddagger - \Delta G^\ddagger}{T_c} = \frac{33,113 - 61,200}{283.15} = \frac{-28,087}{283.15} \approx -99.2\text{ J/(mol}\cdot\text{K)}\]
  • 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.
Intermediate Example 5.5: Stereochemical Double-Inversion Trajectory in the Tsuji-Trost Reaction

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:

  1. Starting material: $(R,E)$-1,3-diphenylallyl acetate. The acetate leaving group ($-\text{OAc}$) resides on one defined face of the allylic plane.
  2. In the oxidative addition step, the palladium(0) catalyst coordinates the double bond and performs a nucleophilic displacement on the acetate-bearing carbon.
  3. This displacement occurs via an outer-sphere inversion pathway: palladium attacks from the face opposite to the leaving acetate group:
\[\text{Step 1: Inversion of Stereochemical Configuration at Carbon}\]
  1. 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):

  1. Dimethyl sodiomalonate is a stabilized carbanion ($\text{p}K_a \approx 13$, soft nucleophile).
  2. 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:
\[\text{Step 2: Second Inversion of Stereochemical Configuration}\]

3. Summing the two elementary steps:

\[\text{Net Stereochemical Trajectory} = \text{Inversion} + \text{Inversion} = \mathbf{Net\ Retention}\]
  1. The product retains the original $(R)$ absolute configuration: $(R,E)$-dimethyl 2-(1,3-diphenylallyl)malonate.

(c) Stereochemical Divergence with Hard Nucleophile ($Me\text{MgBr}$):

  1. Methylmagnesium bromide is a hard, localized carbanion.
  2. Hard nucleophiles cannot perform outer-sphere attack on the external face of the allyl ligand.
  3. Instead, $Me\text{MgBr}$ attacks the electropositive palladium metal center directly via transmetallation:
\[[(\eta^3-\text{allyl})\text{Pd}L_2]^+ + Me\text{MgBr} \longrightarrow [(\eta^3-\text{allyl})\text{Pd}(Me)L_2] + \text{MgBr}^+\]
  1. 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).
  2. Net Stereochemical Trajectory with Hard Nucleophile:
\[\text{Inversion (Oxidative Addition)} + \text{Retention (Reductive Elimination)} = \mathbf{Net\ Inversion}\]
  • Thus, the reaction with $Me\text{MgBr}$ yields the opposite $(S)$ enantiomer!
Intermediate Example 5.6: Alkyne Coordination as 2-Electron vs. 4-Electron Donors in Tungsten Complexes

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 $0$):
\[OS = 0 - [2(-1) + 0 + 0] = +2 \implies \text{W}(\text{II}) (d^4)\]
  • 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
\[VEC = 6 + 2 + 6 + 2 = 16\text{ valence electrons}\]

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:
\[VEC = 6 + 2 + 6 + 4 = \mathbf{18\text{ valence electrons}}\]
  • 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:
\[\delta(^{13}\text{C}) = \mathbf{200 - 240\text{ ppm}}\]

This downfield shift (in the range typical of carbenes and metal-alkylidynes) is the definitive spectroscopic signature of a 4-electron donating alkyne.

Advanced Example 5.7: Frontier Molecular Orbital Derivation of the DGM Rules for Cyclic Polyenes

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:

\[\Delta E = \frac{q_\text{Nu} q_i}{\epsilon R} + 2 \frac{|c_\text{Nu} c_i \beta|^2}{E_\text{LUMO}(\text{complex}) - E_\text{HOMO}(\text{Nu})}\]

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:
\[|c_\text{Nu} c_\text{even} \beta|^2 \gg |c_\text{Nu} c_\text{odd} \beta|^2\]
  • 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.
Advanced Example 5.8: Quantum Mechanics of the $\pi-\sigma-\pi$ Dynamic Fluxional Exchange in $\eta^3$-Allyls

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 $L$:

  1. Let the starting 16-electron complex be $\text{Pd}_{\eta^3}$.
  2. Step 1: Associative Attack of Base $L$:

Incoming base $L$ coordinates to palladium, inducing an $\eta^3 \to \eta^1$ hapticity ring slip:

\[\text{Pd}_{\eta^3} + L \xrightleftharpoons[k_{-1}]{k_1} \text{Pd}_{\eta^1}-L \quad (16\text{-electron } \sigma\text{-allyl intermediate})\]

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 $k_\text{rot}$:

\[\text{Pd}_{\eta^1}-L \xrightleftharpoons[k_\text{rot}]{k_\text{rot}} (\text{Pd}_{\eta^1}-L)'\]

4. Step 3: Dissociation of $L$ and Re-coordination:

\[(\text{Pd}_{\eta^1}-L)' \xrightarrow{k_{-1}} \text{Pd}_{\eta^3}' + L\]

Applying the steady-state approximation to the intermediate $[\text{Pd}_{\eta^1}-L]$:

\[\frac{d[\text{Pd}_{\eta^1}-L]}{dt} = k_1 [\text{Pd}_{\eta^3}][L] - (k_{-1} + k_\text{rot}) [\text{Pd}_{\eta^1}-L] = 0\]
\[[\text{Pd}_{\eta^1}-L] = \frac{k_1 [\text{Pd}_{\eta^3}][L]}{k_{-1} + k_\text{rot}}\]

The observed rate of exchange of syn/anti protons is:

\[R_\text{exchange} = k_\text{rot} [\text{Pd}_{\eta^1}-L] = \frac{k_1 k_\text{rot} [L]}{k_{-1} + k_\text{rot}} [\text{Pd}_{\eta^3}]\]

Thus, the apparent pseudo-first-order rate constant is:

\[k_\text{obs} = \frac{k_1 k_\text{rot} [L]}{k_{-1} + k_\text{rot}}\]

(b) Saturation Kinetic Regimes:

1. At Low Base Concentration or Fast Rotation ($k_{-1} \gg k_\text{rot}$):

\[k_\text{obs} \approx \left(\frac{k_1 k_\text{rot}}{k_{-1}}\right) [L] = K_1 k_\text{rot} [L]\]

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 $k_\text{rot}$:

\[k_\text{obs} \to k_\text{rot}\]

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.
Advanced Example 5.9: Electronic and Bite-Angle Control of Regioselectivity in Asymmetric Allylic Alkylation

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).
  1. 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 $P_2$.
  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.
  3. 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).
  4. Nucleophilic attack by soft carbanions (dimethyl malonate) occurs preferentially at the allyl terminus trans to the stronger $\pi$-acceptor ($P_2$).
  5. 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 $\Delta G_S^\ddagger$:

  1. According to transition-state theory:
\[k_R = \frac{k_B T}{h} \exp\left(-\frac{\Delta G_R^\ddagger}{RT}\right), \quad k_S = \frac{k_B T}{h} \exp\left(-\frac{\Delta G_S^\ddagger}{RT}\right)\]
  1. The enantiomeric ratio ($er$) is:
\[er = \frac{[R]}{[S]} = \frac{k_R}{k_S} = \exp\left(-\frac{\Delta G_R^\ddagger - \Delta G_S^\ddagger}{RT}\right) = \exp\left(\frac{\Delta\Delta G^\ddagger}{RT}\right)\]

where $\Delta\Delta G^\ddagger = \Delta G_S^\ddagger - \Delta G_R^\ddagger > 0$ (assuming $R$ is favored).

  1. The enantiomeric excess ($ee$) is defined as:
\[ee = \frac{[R] - [S]}{[R] + [S]} = \frac{\frac{[R]}{[S]} - 1}{\frac{[R]}{[S]} + 1} = \frac{er - 1}{er + 1}\]
  1. Substituting $er = \exp\left(\frac{\Delta\Delta G^\ddagger}{RT}\right)$:
\[ee = \frac{\exp\left(\frac{\Delta\Delta G^\ddagger}{RT}\right) - 1}{\exp\left(\frac{\Delta\Delta G^\ddagger}{RT}\right) + 1} = \tanh\left(\frac{\Delta\Delta G^\ddagger}{2RT}\right)\]
  • 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!