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SAMEEN FATIMA
TOPIC OF ASSIGNMENT
n-BUTANE AND CYCLOHEXANE
(according to conformational isomerism)
CONFORMATION IN n-BUTANE
When the dihedral angle = 0° or 360°, (syn conformation) in butane,
the two methyl groups are in close proximity with the molecule,
therefore the potential energy is at its highest. In the anticonformation
(when the dihedral angle = 180°) the potential energy is at its lowest,
therefore the most stable.
EXPLANATION
The conformational possibilities increase as alkanes become larger. A
plot of potential energy against rotation about the C(2)–C(3) bond in
butane is shown below. The lowest-energy arrangement, called the
antiperiplanar (or anti) conformation, is the one in which the two large
methyl groups are as far apart as possible. As rotation around the
C(2)–C(3) bond occurs, another eclipsed conformation (anticlinal) is
reached in which there are two Me–H interactions and one H–H
interaction. If we assign the energy value (4 kJ/mol) for H–H eclipsing
interactions that was previously derived from ethane, we can predict
that each Me–H interaction in the anticlinal conformation costs about
5 kJ/mol.
As bond rotation continues, an energy minimum is reached at the
staggered conformation where the methyl groups are 60° apart (a
gauche relationship). This lies 3.2 kJ/mol higher in energy than the anti
conformation even though it has no eclipsing interactions. This energy
difference is due to the fact that the hydrogen atoms of the methyl
groups are near each other in the gauche conformation, resulting in
steric strain, which is the repulsive interaction that occurs when atoms
would otherwise tend to occupy the same space.
As the dihedral angle between the methyl groups approaches 0°, an
energy maximum is reached. The methyl groups are forced even closer
together than in the gauche conformation, and both torsional strain
and steric strain are present. A total strain energy of 25 kJ/mol has
been estimated for this conformation, allowing us to calculate a value
of 17 kJ/mol for the Me–Me eclipsing interaction.
Completing the 360° rotation after the synperiplanar point produces
the mirror images of what we've already seen; another gauche
conformation, another eclipsed conformation and finally a return to
the anti conformation.
Use the interactive model below to explore the conformations of
butane. In particular, try the following 'visualisation' of steric strain:
Select Reset, Atoms 100%, coloured methyls and Animate loop, then
watch the interactions of the two methyl groups as they pass by each
other. The butane structure used in this animation was generated by
quantum chemical calculation using the 6-31G* basis set.
Eclipsed conformations
Totally eclipsed partially eclipsed partially eclipsed
0o (I) 120O (II) 240O (III)
Staggered conformations
IV V VI
60O (gouche) 180o (anti) 300o (gouche)
CONFORMATION IN CYCLOHEXANE
A cyclohexane conformation is any of several three-dimensional shapes
adopted by a cyclohexane molecule. Because many compounds feature
structurally similar six-membered rings, the structure and dynamics of
cyclohexane are important prototypes of a wide range of
compounds.[1][2]
PRINCIPLE CONFORMERS
Chair conformation
The chair conformation is the most stable conformer. At 25 °C, 99.99%
of all molecules in a cyclohexane solution adopt this conformation.
The symmetry is D3d. All carbon centers are equivalent. Six hydrogen
centers are poised in axial positions, roughly parallel with the C3 axis.
Six hydrogen atoms are poised nearly perpendicular to the C3
symmetry axis. These H atoms are respectively referred to as axial and
equatorial.
Each carbon bears one "up" and one "down" hydrogen. The C-H bonds
in successive carbons are thus staggered so that there is little torsional
strain. The chair geometry is often preserved when the hydrogen
atoms are replaced by halogens or other simple groups.
Boat conformation
The boat conformations have higher energy than the chair
conformations. The interaction between the two flagpole hydrogens, in
particular, generates steric strain. Torsional strain also exists between
the C2–C3 and C5–C6 bonds, which are eclipsed. Because of this strain,
the boat configuration is unstable (i.e. is not a local energy minimum).
The symmetry is C2v.
The boat conformations spontaneously distorts to twist-boat
conformations. Here the symmetry is D2, a purely rotational point
group. This conformation can be derived from the boat conformation
by applying a slight twist to the molecule so as to remove eclipsing of
two pairs of methylene groups.
The concentration of the twist-boat conformation at room
temperature is less than 0.1%, but at 1073 kelvins it can reach 30%.
Rapid cooling of a sample of cyclohexane from 1073 K to 40 K will
freeze in a large concentration of twist-boat conformation, which will
then slowly convert to the chair conformation upon heating.
Boat conformation
AXIAL AND EQUILIBRIUM BONDS IN CYCLOHEXANE
The bonds in cyclohexane conformation are shown below in structures.
TWISTED BOAT

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N butane and cyclohexane

  • 1. SAMEEN FATIMA TOPIC OF ASSIGNMENT n-BUTANE AND CYCLOHEXANE (according to conformational isomerism) CONFORMATION IN n-BUTANE When the dihedral angle = 0° or 360°, (syn conformation) in butane, the two methyl groups are in close proximity with the molecule, therefore the potential energy is at its highest. In the anticonformation (when the dihedral angle = 180°) the potential energy is at its lowest, therefore the most stable. EXPLANATION The conformational possibilities increase as alkanes become larger. A plot of potential energy against rotation about the C(2)–C(3) bond in
  • 2. butane is shown below. The lowest-energy arrangement, called the antiperiplanar (or anti) conformation, is the one in which the two large methyl groups are as far apart as possible. As rotation around the C(2)–C(3) bond occurs, another eclipsed conformation (anticlinal) is reached in which there are two Me–H interactions and one H–H interaction. If we assign the energy value (4 kJ/mol) for H–H eclipsing interactions that was previously derived from ethane, we can predict that each Me–H interaction in the anticlinal conformation costs about 5 kJ/mol. As bond rotation continues, an energy minimum is reached at the staggered conformation where the methyl groups are 60° apart (a gauche relationship). This lies 3.2 kJ/mol higher in energy than the anti conformation even though it has no eclipsing interactions. This energy difference is due to the fact that the hydrogen atoms of the methyl groups are near each other in the gauche conformation, resulting in steric strain, which is the repulsive interaction that occurs when atoms would otherwise tend to occupy the same space. As the dihedral angle between the methyl groups approaches 0°, an energy maximum is reached. The methyl groups are forced even closer together than in the gauche conformation, and both torsional strain
  • 3. and steric strain are present. A total strain energy of 25 kJ/mol has been estimated for this conformation, allowing us to calculate a value of 17 kJ/mol for the Me–Me eclipsing interaction. Completing the 360° rotation after the synperiplanar point produces the mirror images of what we've already seen; another gauche conformation, another eclipsed conformation and finally a return to the anti conformation. Use the interactive model below to explore the conformations of butane. In particular, try the following 'visualisation' of steric strain: Select Reset, Atoms 100%, coloured methyls and Animate loop, then watch the interactions of the two methyl groups as they pass by each other. The butane structure used in this animation was generated by quantum chemical calculation using the 6-31G* basis set. Eclipsed conformations Totally eclipsed partially eclipsed partially eclipsed 0o (I) 120O (II) 240O (III) Staggered conformations IV V VI 60O (gouche) 180o (anti) 300o (gouche) CONFORMATION IN CYCLOHEXANE
  • 4. A cyclohexane conformation is any of several three-dimensional shapes adopted by a cyclohexane molecule. Because many compounds feature structurally similar six-membered rings, the structure and dynamics of cyclohexane are important prototypes of a wide range of compounds.[1][2] PRINCIPLE CONFORMERS Chair conformation The chair conformation is the most stable conformer. At 25 °C, 99.99% of all molecules in a cyclohexane solution adopt this conformation. The symmetry is D3d. All carbon centers are equivalent. Six hydrogen centers are poised in axial positions, roughly parallel with the C3 axis. Six hydrogen atoms are poised nearly perpendicular to the C3 symmetry axis. These H atoms are respectively referred to as axial and equatorial. Each carbon bears one "up" and one "down" hydrogen. The C-H bonds in successive carbons are thus staggered so that there is little torsional strain. The chair geometry is often preserved when the hydrogen atoms are replaced by halogens or other simple groups. Boat conformation The boat conformations have higher energy than the chair conformations. The interaction between the two flagpole hydrogens, in particular, generates steric strain. Torsional strain also exists between the C2–C3 and C5–C6 bonds, which are eclipsed. Because of this strain, the boat configuration is unstable (i.e. is not a local energy minimum). The symmetry is C2v.
  • 5. The boat conformations spontaneously distorts to twist-boat conformations. Here the symmetry is D2, a purely rotational point group. This conformation can be derived from the boat conformation by applying a slight twist to the molecule so as to remove eclipsing of two pairs of methylene groups. The concentration of the twist-boat conformation at room temperature is less than 0.1%, but at 1073 kelvins it can reach 30%. Rapid cooling of a sample of cyclohexane from 1073 K to 40 K will freeze in a large concentration of twist-boat conformation, which will then slowly convert to the chair conformation upon heating. Boat conformation AXIAL AND EQUILIBRIUM BONDS IN CYCLOHEXANE The bonds in cyclohexane conformation are shown below in structures. TWISTED BOAT