Organic Chemistry · Organic Compounds: Cycloalkanes and Their Stereochemistry
Conformations of Cyclohexane
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In 30 seconds
Cyclohexane (C6H12) is the ring chemists study more than any other because it can escape ring strain entirely. A six-membered ring made of tetrahedral carbons cannot lie flat: a planar hexagon would force 120° bond angles onto carbons that prefer 109.5°, and every C–H bond would eclipse its neighbor. Instead, the ring puckers into a chair shape in which every bond angle is near the tetrahedral ideal and every bond is staggered. This topic maps the conformations of cyclohexane — chair, boat, Twist-boat Boat twisted to stagger bonds and spread flagpole hydrogens Full entry →, and Half-chair Shape with one carbon out of the plane of the other five Full entry → — and the Ring flip Chair-to-chair interconversion through half-chair and boat states Full entry → that interconverts the two chair forms. The chair's strain-free geometry is the foundation for axial/equatorial bonds, substituent preferences, and fused-ring conformations later in this chapter.
Why this matters
Cyclohexane rings are everywhere in chemistry beyond the classroom. Steroid hormones, cholesterol, many drugs, and countless natural products are built from cyclohexane rings fused together, and a molecule's three-dimensional shape controls how it binds a receptor or how fast it reacts. On exams, conformational analysis is a predictable source of points: ranking conformations by strain, drawing the chair correctly, and explaining why the ring flips are core skills. In drug design, replacing a flat aromatic ring with a saturated ring changes solubility, metabolism, and shape, so medicinal chemists reason in exactly these terms.
The college version
Core Concepts
Why a planar hexagon fails
All six carbons of cyclohexane are sp3-hybridized and prefer tetrahedral 109.5° bond angles. A flat, regular hexagon has 120° internal angles, so forcing the ring planar would compress every C–C–C angle — that is Angle strain Energy cost of bond angles forced away from the tetrahedral ideal Full entry → — and would also put the C–H bonds on adjacent carbons in eclipsed positions, adding Torsional strain Energy cost of eclipsed bonds Full entry →. A planar cyclohexane would be far too high in energy to exist. The ring's answer is to pucker: bending out of plane lets the angles relax toward 109.5° and lets the bonds stagger.
The chair conformation
The chair is the shape that satisfies both demands. Picture a carbon 1 raised above the average plane, carbon 4 below it, and the other four carbons arranged between them. In this geometry every C–C–C angle is 109.5° (no angle strain), and a Newman projection down any C–C bond shows three perfectly staggered pairs of bonds (no torsional strain). There are no close nonbonded contacts either, so the chair has essentially zero ring strain — the energy minimum for the ring.
Boat, twist-boat, and half-chair
The boat Conformation Any arrangement of atoms reached by rotating single bonds without breaking bonds Full entry → has both C1 and C4 on the same side of the plane. It is not badly angle-strained, but it pays twice: the C2–C3 and C5–C6 bonds are eclipsed, and the hydrogens on C1 and C4 point toward each other — the flagpole interaction — adding steric strain. The boat sits about 29 kJ/mol (7 kcal/mol) above the chair. Twisting the boat slightly gives the twist-boat, which staggers the eclipsed bonds and spreads the flagpole hydrogens apart, dropping the energy to about 23 kJ/mol above the chair. The half-chair has one carbon lifted out of the plane of the other five; it is the highest point on the flip pathway, about 45 kJ/mol above the chair.
The ring flip
The ring flip converts one chair into the other without breaking any bonds. The pathway climbs over the half-chair, passes through a boat, and settles into the opposite chair. For unsubstituted cyclohexane the two chairs are identical in energy, so the flip is degenerate. The barrier is only about 45 kJ/mol, so at room temperature the ring flips millions of times per second. As a preview of the next topic, the flip swaps axial and equatorial positions.
Common Confusions
| Do Not Confuse | With | Difference |
|---|---|---|
| Chair conformation | Flat hexagon drawing | The chair is puckered in 3-D; a flat hexagon implies 120° angles and eclipsed bonds that real cyclohexane never has |
| Boat | Chair | Boat has eclipsed bonds and flagpole hydrogens; it is ~29 kJ/mol less stable |
| Ring flip | Re-drawing the ring | The flip is a real conformational change through half-chair and boat; the paper drawing just shows the result |
| Twist-boat | Boat | Twist-boat is twisted to remove eclipsing, so it is ~6 kJ/mol more stable than the boat |
| Cyclohexane chair | Benzene ring | Benzene is planar and aromatic with sp2 carbons; cyclohexane is puckered with sp3 carbons |

Eli explains
The same idea, in plain words
Explain it like I’m 10
A drawing of a hexagon looks flat, but a real cyclohexane molecule bends like a folding chair so its six corners don't all sit in one plane. The bent chair shape lets every bond relax into a comfortable staggered position, like six friends in a circle turning so nobody's elbows bump. The molecule can bend into the opposite chair and back, and it does this millions of times each second at room temperature.
Worked example
Example 1: Ranking the conformations with the three strain types
Walk through the reasoning that concludes the chair wins. Start with the chair and ask what strain could possibly remain: angles are 109.5° (no angle strain), every C–C bond viewed end-on is staggered (no torsional strain), and no hydrogens crowd each other (no steric strain). Now try the boat: angles are close to tetrahedral, so angle strain is still small, but look down the C2–C3 bond — the hydrogens are eclipsed, adding torsional strain — and the C1 and C4 hydrogens point straight at each other, adding steric strain. The boat pays roughly 29 kJ/mol for those penalties. The twist-boat staggers the eclipsed bonds and rotates the flagpole hydrogens apart, recovering most of that cost, which is why twist-boat (23 kJ/mol) sits below boat (29 kJ/mol). The verdict: chair first, twist-boat second, boat third, half-chair last.
Example 2: Following a ring flip from chair to chair
Label the six carbons 1–6 around the ring, with C1 and C4 opposite each other. In chair A, C1 is above the average plane and C4 is below. To flip, C1 swings down and C4 swings up: the ring passes through the half-chair (one carbon in the plane of the other five), then through a boat (C1 and C4 both near the same side), then through a second twist-boat, then the second half-chair, and finally chair B, in which C1 is below and C4 is above. Every C–C bond rotated along the way, yet no bond broke. Because the two chairs are mirror-related but identical in energy for unsubstituted cyclohexane, the equilibrium constant is 1 — the molecule spends equal time in each.
Key takeaways
- The chair is the energy minimum: no angle strain (109.5° angles), no torsional strain (all bonds staggered), no flagpole steric strain.
- Energy ladder above the chair: twist-boat ≈ 23 kJ/mol, boat ≈ 29 kJ/mol, half-chair ≈ 45 kJ/mol (commonly taught reference values).
- The half-chair is the transition state for the ring flip, not an isolable conformation.
- A planar hexagon would force 120° angles onto sp3 carbons — never draw it as a real structure.
- The two chairs of unsubstituted cyclohexane are identical (degenerate) and interconvert rapidly at room temperature.
- Newman projection rule: along any C–C bond of the chair, the three bonds are fully staggered.
Check yourself
6 review questions from the chapter. Try each one, then open the answer.
Why can't cyclohexane exist as a planar hexagon?
Show answer
A planar hexagon would force 120° bond angles onto tetrahedral (sp³) carbons, adding angle strain, and would put every C–H bond eclipsed, adding torsional strain.
Which conformation of cyclohexane is the global energy minimum, and what strain types does it avoid?
Show answer
The chair: it has 109.5° angles (no angle strain), fully staggered bonds (no torsional strain), and no flagpole interactions (no steric strain).
About how much energy separates the chair from the boat, and what two interactions does the boat pay for?
Show answer
About 29 kJ/mol; the boat pays torsional strain from eclipsed C2–C3 and C5–C6 bonds plus steric strain from the flagpole hydrogens on C1 and C4.
What conformation sits at the top of the ring-flip barrier?
Show answer
The half-chair, roughly 45 kJ/mol above the chair.
Are the two chair conformations of unsubstituted cyclohexane the same or different in energy?
Show answer
Identical — the two chairs of unsubstituted cyclohexane are degenerate, so the flip equilibrium constant is 1.
Through which conformation do the two twist-boat forms interconvert?
Show answer
Through the boat conformation, which is the transition state connecting the two twist-boats.
Study tools & related lessonsKey vocabulary · Related
Key vocabulary
- Conformation
- Any arrangement of atoms reached by rotating single bonds without breaking bonds
- Chair conformation
- Puckered cyclohexane shape with all angles near 109.5° and all bonds staggered
- Boat conformation
- Puckered shape with C1 and C4 on the same side; eclipsed bonds and flagpole H's
- Twist-boat
- Boat twisted to stagger bonds and spread flagpole hydrogens
- Half-chair
- Shape with one carbon out of the plane of the other five
- Ring flip
- Chair-to-chair interconversion through half-chair and boat states
- Angle strain
- Energy cost of bond angles forced away from the tetrahedral ideal
- Torsional strain
- Energy cost of eclipsed bonds
Sources & references
This lesson was adapted from the open educational references above; their licenses and attributions are preserved. See Copyright & Licensing.
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