Rings are everywhere in organic chemistry — in sugars, steroids, alkaloids, and a large fraction of pharmaceuticals — and six-membered rings dominate the list. The reason is worth understanding rather than accepting: six carbons is the ring size at which a closed loop can satisfy every geometric demand at once, and no other small ring can.
Three kinds of ring strain
Angle strain is the cost of forcing bond angles away from their ideal value — about 109.5° for sp³ carbon. A ring's geometry can impose an angle, and if that angle is wrong the orbitals overlap poorly and the bonds are weakened.
Torsional strain is the cost of eclipsing bonds, exactly as in the Newman projections of the previous section. A flat ring forces every adjacent pair of substituents into an eclipsed relationship, because there is no way to stagger them while staying planar.
Steric strain is the cost of non-bonded atoms bumping into each other through space — van der Waals repulsion. This is the gauche interaction from butane, and on a cyclohexane ring it takes the specific form of a 1,3-diaxial interaction, which the next section covers.
These three are independent, they can trade off against each other, and a ring's total strain is what you get after the molecule has found the compromise that minimizes their sum.
Small rings pay these costs differently
| Ring | Total strain | Dominant problem |
|---|---|---|
| cyclopropane | 27.5 | angle (60°) + fully eclipsed |
| cyclobutane | 26.3 | angle (~88°) + torsional |
| cyclopentane | 6.2 | torsional, mostly relieved |
| cyclohexane | 0 | none |
| cycloheptane | 6.2 | torsional + transannular |
Cyclopropane is a flat triangle by geometric necessity — three points define a plane — so it is stuck with 60° bond angles against an ideal of 109.5°, and with every C–H bond eclipsing its neighbor. Its bonds are so distorted that they are often described as "bent" or banana bonds, with the electron density bulging outside the internuclear lines. This is why cyclopropanes undergo ring-opening reactions that no ordinary alkane would.
Cyclobutane could be planar at 90° angles, which would be less angle strain than cyclopropane. Instead it puckers slightly, accepting worse angles (about 88°) in exchange for relieving some of the eclipsing. That trade — worse angle strain to buy relief from torsional strain — tells you that torsional strain is not a minor effect.
Cyclopentane puckers into an "envelope" shape, with four carbons roughly coplanar and the fifth out of plane. Its angles in a planar form would be 108°, essentially ideal, so it has almost no angle strain to begin with; the puckering is purely to reduce eclipsing, and it leaves a modest residual strain.
Why the chair works
Two conditions have to be met simultaneously, and the chair meets both exactly.
Angles. Every C–C–C angle in a chair is about 111°, within two degrees of ideal tetrahedral. Essentially no angle strain.
Torsion. Sight down any ring C–C bond of a chair and you get a perfectly staggered Newman projection — all dihedral angles 60°, no eclipsing anywhere in the ring. Essentially no torsional strain.
Satisfying either condition alone is easy; satisfying both at once is what requires six carbons and a pucker. Five is too few and seven starts to introduce clashes across the ring. That coincidence of geometry is why six-membered rings are so overwhelmingly common in nature and in drug molecules.
Drawing a chair that works
A drawable chair is a skill worth ten minutes of deliberate practice, because a badly drawn chair makes every axial/equatorial judgement afterwards unreliable. The reliable method: draw two parallel lines offset from each other, then connect their ends with two more pairs of parallel lines, so that the finished shape has three sets of two parallel lines. If your drawing does not have that property, it is not a chair, and the substituent directions will not come out right.
The single most useful check is that the two "ends" of the chair point in opposite directions — one carbon up, one carbon down, with the four in between forming a plane. Rotating a real model or using the 3D viewer tool for a minute does more for this than any amount of reading.
The other conformations
The chair is the global minimum, but it is not the only shape cyclohexane can adopt. The boat conformation, about 6.5 kcal/mol above the chair, suffers from eclipsing along two of its bonds and from a "flagpole" interaction between the two hydrogens at the raised ends. The twist-boat, about 5.5 kcal/mol up, relieves some of that by twisting, and is a genuine shallow minimum rather than a transition state — the high point a molecule passes through on the way between two shapes, never something it sits in. The half-chair, around 10–11 kcal/mol up, is the actual transition state between chair forms.
In unsubstituted cyclohexane, over 99% of molecules are in a chair at any moment. The other conformations matter mainly as waypoints on the ring-flip pathway, which is the subject of two sections from here.
What carries forward
The chair conformation is the setting for everything in the rest of this chapter, and the axial/equatorial distinction that follows from it governs the reactivity of every substituted six-membered ring you will meet. In Module 6 it determines which E2 eliminations are geometrically possible at all. In Module 8, the ring strain of a three-membered ring is what makes epoxides so much more reactive than ordinary ethers — the same strain arithmetic, put to work.