DEE shows larger charge transfer per molecule than THF: DEE is a better electron donor per O atom, but THF compensates with higher coordination number.
Reliability Assessment
Grade Distribution
A True minimum (0 imag)
13
A- Quasi-minimum (< -10 cm-1)
1
B Small imag (< -30 cm-1)
2
C Significant imag
0
81% Grade A. All B grades have imaginary frequencies < -25 cm-1 (quasi-RRHO threshold).
Methodology Validation
Functional
wB97X-D3 (range-separated hybrid + D3)
Basis Set
def2-TZVP (triple-zeta)
Dispersion
Built-in D3 correction
Thermochemistry
Quasi-RRHO (Grimme, B_av)
SCF Convergence
TightSCF (1e-8 Eh)
RI Approximation
RIJCOSX / def2/J
Known Limitations
Gas-phase calculations (no implicit solvent model)
Single conformer per cluster (no conformational averaging)
DEE steric constraint: max 2-coordinate (DEE3, DEE4 excluded)
BSSE not explicitly corrected (mitigated by TZVP basis)
Reoptimization Log
Li(THF)1
Disp reopt → true minimum
A
Li(THF)2
Reopt → true minimum
A
Li(THF)4
Reopt → true minimum (dG shift: -8 kcal/mol)
A
Li(FSI)(THF)3
Reopt → true minimum (new CIP)
A
Scientific Discussion
1. Solvation Thermodynamics: THF Always Wins
At 233K, THF forms dramatically stronger solvation shells than DEE. For n=2: DDG = -24.5 kcal/mol in THF's favor. The cyclic rigidity of THF allows efficient packing around Li+ (up to 4-coordinate), while DEE's linear flexibility causes steric exclusion beyond n=2. This asymmetric coordination capacity is the fundamental structural difference.
2. TTE Effect: Entropy-Driven Destabilization
TTE systematically weakens solvation (dG becomes less negative) through massive entropy penalties. Li(THF)2(TTE)2 has dG = +3.65 kcal/mol (thermodynamically unfavorable) despite dH = -30.85 kcal/mol. The TdS penalty scales with TTE count: -16.5 (1 TTE) → -28.8 (2 TTE) → -34.5 kcal/mol (2 TTE + 2 solvent). This confirms TTE's role as a non-coordinating diluent that creates entropy-driven lability in the solvation shell.
3. The Barrier Paradox: Weaker Binding, Higher Barrier?
Preliminary Phase 3 data reveals a counterintuitive trend: DEE desolvation barriers (17.0 kcal/mol) are significantly higher than THF (6.7 kcal/mol), despite DEE having weaker binding. Two hypotheses: (1) DEE's linear geometry creates a conformational trap — the transition state requires an unfavorable geometry that cyclic THF avoids, or (2) the Li-O(TTE) interaction provides a better relay for THF displacement. CIP barriers show a similar but reduced trend (9.9 vs 5.6 kcal/mol), suggesting FSI- partially compensates.
4. Entropy as the Hidden Variable
Temperature dependence analysis shows dG shifts 8-12 kcal/mol between 298K and 223K for TTE-containing clusters. The implication: at low temperature, entropy penalties decrease, making the TTE-disrupted shells relatively more stable. This means the LHCE design principle (TTE dilution) becomes less effective at low T. The practical consequence: DEE's inherently weaker binding (less entropy penalty at low T) may translate to easier desolvation kinetics despite the paradoxical PES barrier.
Progress 72%
Phase 1: Monomer Optimization
5/5 (100%)
Phase 2: Solvation Clusters
16/16 (100%) + 5 CIP
Phase 3: Desolvation PES Scans
6/10 complete (60%)
Currently Running
Calculation
PID
Progress
Notes
DEE2_TTE1 remove DEE (FIX v2)
391599
Step 1/20
Model Hessian, conservative step. Fixed .carthess bug.