Skeletal structure
The slider turns the C3 half of the molecule about the C2–C3 bond as a rigid body. Bond lengths and bond angles never change; only the dihedral does.
Dihedral angle C1–C2–C3–C4
180°anti
Energy along the rotation
Relative energy0.0 kcal/mol
Strain termsnone
C1···C4 distance
Closest H···H between the methyls
Stationary-point energies are the textbook additive values (McMurry): H/H eclipsing 1.0, H/CH3 eclipsing 1.4, CH3/CH3 eclipsing 2.5, gauche 0.9 kcal/mol. The curve between them is a smooth interpolation, not a calculation. Two hydrogens closer than 2.4 Å (their van der Waals contact distance) are shown in red.
Newman projection (live)
front C2, back C3
| anti (180°) | 0 |
| gauche (60°, 300°) | 0.9 |
| eclipsed H/CH3 (120°, 240°) | 3.8 |
| eclipsed CH3/CH3 (0°) | 4.5 |
kcal/mol relative to anti
Let it relax
At 180°, 60°, 120° or 0°, Optimize moves the model to its quantum-chemical geometry (ORCA, r2SCAN-3c, started from the ideal structure; the two eclipsed conformers with the C1–C2–C3–C4 dihedral held). Notice how the methyls lean apart at 0° and how the gauche dihedral opens beyond 60°. Back to ideal restores the construction.
Exercise: count the gauche interactions
Ideal geometry used in the model
| C–C bond length | 1.54 Å |
| C–H bond length | 1.09 Å |
| Every bond angle | 109.47° |
| Dihedrals not on the C2–C3 axis | ±60° / 180° |
At 180° the whole molecule lies on the diamond lattice. The header badge re-checks every bond, angle, and dihedral each time the slider moves.
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C H
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