Inorganic Chemistry
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that R2Zn should become more Lewis acidic, leading to
stronger binding of added ligands, for example, the nitrogen
donors in a “C2ZnN2” complex.
Lewis acidity is typically quantified using adduct formation
thermodynamics, where an acid would be considered more
Lewis acidic if formation of the acid−base adduct (keeping the
base constant) is thermodynamically more favorable.15 The
change in the thermodynamic Lewis acidity resulting from C−
Zn−C bending is demonstrated with density functional theory
(DFT), where we used TPSSTPSS/cc-pVTZ, known to be
excellent for zinc.16 The C−Zn−C angle was fixed, and all
other geometric parameters were relaxed (constrained
geometry optimization) in Me2Zn and its two ammonia
adducts Me2Zn(NH3) and Me2Zn(NH3)2. When the C−Zn−
C angle was narrowed from 180° to 147.9° [computed
equilibrium C−Zn−C bond angle for Me2Zn(NH3)2], the
binding energy of the first NH3 fell from −5.29 to −11.31
kcal/mol, while the binding energy of the second NH3 fell
from −3.87 to −7.22 kcal/mol. The trend continued
consistently for 120° and 90° (Table 1). A constrained
Figure 2. LUMO energy changes for the free Me2Zn fragment (top)
and geometry changes for Me2Zn(bipy) (bottom), upon variation of
an enforced C−Zn−C bond angle (TPSSTPSS/cc-pVTZ).
Table 1. Calculated (TPSSTPSS/cc-PVTZ)
Thermodynamic Parameters for the First and Second
Ammonia Binding Events to a ZnMe2 Fragment (Enforced
C−Zn−C Angle)
Me2Zn fragment. While Zn−N strengthening upon C−Zn−C
narrowing is also predicted from the MO diagram of four-
coordinate zinc,19 we find that analyzing the two-coordinate
Me2Zn fragment provides the simplest explanation. As another
effect, upon narrowing of C−Zn−C, the C−Zn distance
slightly elongates (Figure 2, bottom), also predicted (ψ2
becomes more antibonding).
second binding event
first binding event (kcal/mol)
(kcal/mol)
C−Zn−
C angle
(deg)
ΔE
ΔH
ΔG
3.30
−4.04
−8.24
ΔE
ΔH
ΔG
180
147.9
120
90
−5.29
−11.31
−17.60
−23.86
−5.88
−11.91
−18.19
−24.45
−3.87
−7.22
−8.89
−4.46
−7.81
−9.48
3.30
0.3
−2.48
−4.14
Given the wealth of crystallographic data available now, a
structure correlation study involving experimental structures is
timely. For zinc dialkyls, diaryls, or dialkenyls R2Zn(“N2”) with
“N2” = bipy, several crystal structures are known, namely, the
structures that have R = 1-adamantyl and 2-adamantyl,
reported recently,20 as well as older reports with R = methyl,21
1-methylvinyl and 2,2-dimethylvinyl,22 and bis(trimethylsilyl)-
methyl.3 We are adding the characterization of cyclopentyl2Zn-
(bipy) (1) and phenyl2Zn(bipy) (2). Using a common
derivative of bipy, 4,4′-di-tert-butyl-2,2′-bipyridine (tBu2-
bipy), we are adding the characterization of neophyl2Zn-
(tBu2-bipy) (3; neophyl = 2-methyl-2-phenylpropyl),
cyclohexyl2Zn(tBu2-bipy) (4), nBu2Zn(tBu2-bipy) (5), 1-
adamantyl2Zn(tBu2-bipy) (6), tBu2Zn(tBu2-bipy) (7), and
cyclopentyl2Zn(tBu2-bipy) (8). The ethyl complexes Et2Zn-
(tBu2-bipy)23 (9) and Et2Zn(bipy)24 (10) are already known
and were additionally characterized here with reduced R1
factor (1.8% versus 2.2% and 2.0% versus 6.1%, respectively).
The structures of 1−10 (see the SI) were included (PreQuest,
version 5.34) in a database search that was run using ConQuest
(version 2.0.2) on the CSD (version 5.40, updates up to May
2019).25 The search was open to all “C2ZnN2” structures with
four-coordinate zinc, including examples containing two
monodentate nitrogen ligands (not just chelates) as well as
carbon ligands other than alkyl/aryl/alkenyl. In total, 161
crystal structures were retrieved, each with the bond distances
and angles around zinc shown in Figure 3. All permutations of
labels were included, to remove the arbitrariness of atom
labeling. A linear plot of the Zn−N distance versus C−Zn−C
angle (see the SI; R2 = 0.49) yields that, over the full range
90−180°, for every 10° of C−Zn−C narrowing, the Zn−N
distance shortens by 0.055 Å, in good agreement with the
computational result (0.048 Å). A linear plot using the new
−14.13
−10.93
−11.52
geometry optimization is artificial, but the predictive power is
real: if the C−Zn−C angle can be forced to be narrow, e.g., in
a metallacycle, the zinc center is predicted to bind ligands
more strongly. The existence of this causal link does not
preclude that the opposite also holds (pushing a donor ligand
closer to zinc bends the C−Zn−C bond). The C−Zn−C angle
and Zn−N distance changes are coupled.17
To shift focus toward synthetically more practical ligands
than NH3, another constrained geometry optimization was
performed on Me2Zn(bipy) (bipy = 2,2′-bipyridine), a
“C2ZnN2” complex prototypical for zinc dialkyls with N-
chelates, compounds easily synthesized and structurally
characterized. In the regime of modest distortions around
tetrahedral geometry, for every 10° of C−Zn−C narrowing,
the Zn−N distance shortens by 0.027 Å (Figure 2, bottom).
The slope is steeper at large angles, and for the range 90−180°,
the overall bond length change is 0.434 Å, corresponding to
0.048 Å per 10°. The LUMO energy of the underlying Me2Zn
fragment is also shown in Figure 2 (top). The computed
symmetries and qualitative appearances shown in Figure 1 and
respond to bending as predicted. The LUMO is essentially the
antibonding component of a 3c-4e interaction.18 The LUMO
energy (Figure 2, top) falls by an impressive 2.12 eV over the
range 180−90° and, in the vicinity of tetrahedral geometry, by
0.24 eV for every 10° of C−Zn−C narrowing, drastically
enhancing the Lewis acidity of the zinc center and
strengthening the interaction between donor atoms and the
B
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