WOBBLcaffeine

IR spectrum look like caffeine

Report
2026-10-15 19:06
OK

caffeine (C8H10N4O2, 194.19 g/mol), by GFN2-xTB: its strongest IR band is at 1712 cm-1, the C=O stretch, its dipole is 3.98 D, dissolving in water is worth -43.9 kJ/mol. At 298 K its entropy is 470.8 J/(mol K) and its heat capacity 211.0 J/(mol K).

dipole
3.98 D
strongest IR band
1712 cm-1
HOMO-LUMO gap
3.40 eV
entropy at 298 K
470.8 J/(mol K)

Confidence high

  • passed geometry convergence, minimum, SCF convergence

Simulation

Infrared spectrum from GFN2-xTB, broadened by 20 cm-1
Infrared spectrum from GFN2-xTB, broadened by 20 cm-1

Checks

statuscheckresult
passgeometry convergenceGFN2-xTB stopped after 18 steps with the largest force at 0.0029 eV/A, under the 0.003 eV/A it aims for
passminimumall 66 frequencies are real, so the structure is a true minimum, after following 1 imaginary mode downhill
passSCF convergenceall 612 GFN2-xTB single points converged within 300 iterations
infothermochemistryideal gas at 298 K and 101 kPa with a rotational symmetry number of 1, and 4 soft modes under 100 cm-1 treated as hindered rotors

Properties

energy-42.154507 Eh (GFN2-xTB)
dipole3.977 D
HOMO and LUMO-10.59 eV and -7.19 eV
zero point energy478.71 kJ/mol
H, S and G at 298 K516.53 kJ/mol, 470.81 J/(mol K) and 376.16 kJ/mol above the electronic energy
heat capacity Cp211.02 J/(mol K)
solvation in water-43.9 kJ/mol

Strongest IR bands

cm-1km/molmode
66642.7N-C-H bend
69156.6N-C-H bend
99047.1N-C-H bend
103457.4N-C-H bend
123339.2C-N stretch
124847.7N-C-H bend
132291.5C-N stretch
1450136.7H-C-H bend
1525142.9N-C-H bend
1578214.8C-N stretch
1712996.4C=O stretch
1733482.8C=O stretch

Assumptions

  1. caffeine as RDKit ETKDG distance geometry relaxed with MMFF94, the lowest of 1 conformers, refined with GFN2-xTB, good to about 0.02 A in bond lengths, 2.5 degrees in angles and 8% in frequencies.
  2. One molecule in the gas phase unless a solvent is named, and a solvent is a continuum (ALPB) rather than explicit molecules.
  3. Thermochemistry treats the molecule as an ideal gas, a rigid rotor and harmonic oscillators, with modes under 100 cm-1 blended into free rotors.
  4. The HOMO-LUMO gap from GFN2-xTB is a trend only, often off by over 1 eV, so it is not an optical gap.