Conformational Analysis

Turn ethane and butane about a C–C bond or flip a cyclohexane chair, and see how strain sets the energy, the barriers and the conformer populations.

Conformation Explorer
Molecule
Units
Cyclohexane
Chair
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AxialEquatorialIn between
AntiGaucheEclipsedOtherCH₃···CH₃ contact
Energy along the inversion
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Here
0
Barrier from chair
0
Barrier from chair′
0
Ring geometry
Puckering Q
θ
φ
C–C–C angles
Chair vs chair′ strain
kcal/mol
Equilibrium
ΔG° chair → chair′
K = [chair′]/[chair]
Chair Chair′
Rate
Average lifetime (1/k)
K = e−ΔG°/RT · k = (kBT/h)e−ΔG‡/RT · R = 8.314 J mol⁻¹ K⁻¹
What to notice
About the model, the numbers, and what to notice

Bond rotation (ethane, butane)

The rotating C–C bond is held at 1.53 Å with tetrahedral groups on each carbon, and only the dihedral angle changes. The strain at 0°, 60°, 120° and 180° is the sum of the interaction costs in the table. The energy curve is a three-term cosine series, E = c + a cos φ + b cos 2φ + d cos 3φ, fit exactly through those four points. For butane, both gauche forms (g⁺ and g⁻) are counted, so K = [gauche]/[anti] = 2e−ΔG°/RT. Rates use the Eyring equation, k = (kBT/h)e−ΔG‡/RT, treating the barrier from the curve as ΔG‡ with a transmission coefficient of 1, so they are order-of-magnitude estimates.

Ring geometry

Ring shapes come from Cremer–Pople puckering coordinates (amplitude Q, angles θ and φ). θ = 0° is the chair and θ = 180° the flipped chair. At θ = 90° the boats (φ = 0°, 60°, …) and twist-boats (φ = 30°, 90°, …) sit on a pseudorotation circle. The path runs chair → half-chair (θ ≈ 51°) → twist-boat → boat → twist-boat → half-chair → chair′, with every C–C bond scaled to an average of 1.53 Å and C–H at 1.09 Å. Substituent directions are tetrahedral at each ring carbon. A bond is drawn axial when it lies within about 35° of the ring normal and equatorial when it lies more than 60° from it.

Energy profile

The curve is a smooth schematic through the stationary points below. Its maxima and minima sit at the named conformations, but its shape between them is not a computed potential energy surface. For substituted rings, the difference in chair strain is blended in across the path.
Bond-rotation interactionStrain used
H/H eclipsed1.0 kcal/mol (4.0 kJ/mol)
CH₃/H eclipsed1.4 kcal/mol (6.0 kJ/mol)
CH₃/CH₃ eclipsed2.6 kcal/mol (11 kJ/mol)
Ethane barrier (3 × H/H)3.0 kcal/mol (12 kJ/mol)
Butane 120° eclipsed / 0° fully eclipsed3.8 / 4.6 kcal/mol (16 / 19 kJ/mol)
Cyclohexane conformationEnergy above chair
Half-chair (transition state)10.8 kcal/mol (45 kJ/mol)
Boat6.9 kcal/mol (29 kJ/mol)
Twist-boat (intermediate)5.5 kcal/mol (23 kJ/mol)
InteractionStrain used
CH₃/H 1,3-diaxial (each)0.87 kcal/mol (3.6 kJ/mol)
Axial CH₃ (A-value, 2 × above)1.74 kcal/mol (7.3 kJ/mol)
CH₃/CH₃ gauche0.9 kcal/mol (3.8 kJ/mol)
These are standard teaching values. Measured barriers and A-values vary slightly with method and solvent. Gas-phase measurements put the butane anti–gauche difference somewhat lower, near 0.6–0.7 kcal/mol. Sources: J. D. Kemp & K. S. Pitzer, J. Chem. Phys. 1936, 4, 749 (ethane barrier); W. A. Herrebout et al., J. Phys. Chem. 1995, 99, 578 (butane); J. McMurry, Organic Chemistry (Cengage), interaction increments; E. L. Eliel & S. H. Wilen, Stereochemistry of Organic Compounds (Wiley, 1994); F. A. L. Anet & A. J. R. Bourn, J. Am. Chem. Soc. 1967, 89, 760; M. Squillacote et al., J. Am. Chem. Soc. 1975, 97, 3244.