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# Dihedral angle

This page is a soft redirect.Dihedral]].

In geometry, a **dihedral** or **torsion angle** is the angle between two hyperplanes.

The dihedral angle of two planes can be seen by looking at the planes "edge on", i.e., along their line of intersection. The dihedral angle <math>\varphi_{AB}</math> between two planes denoted A and B is the angle between their two normal unit vectors <math>\mathbf{n}_{A}</math> and <math>\mathbf{n}_{B}</math>:

- <math>\cos \left(\varphi_{AB}\right) = \mathbf{n}_A \cdot \mathbf{n}_B</math>

A dihedral angle can be signed; for example, the dihedral angle <math>\varphi_{AB}</math> can be defined as the angle through which plane A must be rotated (about their common line of intersection) to align it with plane B. Thus, <math>\varphi_{AB} \;=\; -\varphi_{BA}</math>. For precision, one should specify the angle or its supplement, since both rotations will cause the planes to coincide.

In higher dimension, a *dihedral angle* represents the angle between two hyperplanes.^{[1]}

## Contents

## Alternative definitions

Since a plane can be defined in several ways (e.g., by vectors or points in them, or by their normal vectors), there are several equivalent definitions of a dihedral angle.

Any plane can be defined by two non-collinear vectors lying in that plane; taking their cross product and normalizing yields the normal unit vector to the plane. Thus, a dihedral angle can be defined by four, pairwise non-collinear vectors.

We may also define the dihedral angle of *three* non-collinear vectors <math>\mathbf{b}_1</math>, <math>\mathbf{b}_2</math> and <math>\mathbf{b}_3</math> (red, green and blue, respectively, in the diagram). The vectors <math>\mathbf{b}_1</math> and <math>\mathbf{b}_2</math> define the first plane, whereas <math>\mathbf{b}_2</math> and <math>\mathbf{b}_3</math> define the second plane. The dihedral angle corresponds to an exterior spherical angle, given by

- <math>

\varphi = \operatorname{atan2} \left( \left([\mathbf{b}_1 \times \mathbf{b}_2]\times [\mathbf{b}_2 \times \mathbf{b}_3]\right) \cdot \frac{\mathbf{b}_2}{|\mathbf{b}_2|}, [\mathbf{b}_1 \times \mathbf{b}_2] \cdot [\mathbf{b}_2 \times \mathbf{b}_3] \right),
</math>
as derived in.^{[2]}

## Dihedral angles in polyhedra

Every polyhedron, regular and irregular, convex and concave, has a dihedral angle at every edge.

A dihedral angle (also called the face angle) is the internal angle at which two adjacent faces meet. An angle of zero degrees means the face normal vectors are antiparallel and the faces overlap each other (Implying part of a degenerate polyhedron). An angle of 180 degrees means the faces are parallel (like a tiling). An angle greater than 180 exists on concave portions of a polyhedron.

Every dihedral angle in an edge-transitive polyhedron has the same value. This includes the 5 Platonic solids, the 4 Kepler–Poinsot polyhedra, the two quasiregular solids, and two quasiregular dual solids.

## Dihedral angles of four atoms

The structure of a molecule can be defined with high precision by the dihedral angles between three successive chemical bond vectors. The dihedral angle <math>\varphi</math> varies only the distance between the first and fourth atoms; the other interatomic distances are constrained by the chemical bond lengths and bond angles.

To visualize the dihedral angle of four atoms, it's helpful to look down the second bond vector, which is equivalent to the Newman projection in chemistry. The first atom is at 6 o'clock, the fourth atom is at roughly 2 o'clock and the second and third atoms are located in the center. The second bond vector is coming out of the page. The dihedral angle <math>\varphi</math> is the counterclockwise angle made by the vectors <math>\mathbf{b}_1</math> (red) and <math>\mathbf{b}_3</math> (blue). When the fourth atom eclipses the first atom, the dihedral angle is zero; when the atoms are exactly opposite, the dihedral angle is 180°.

### Improper dihedral angle

An **"improper" dihedral angle** is a similar geometric analysis of four atoms, but typically involves a central atom with three others attached to it rather than the standard arrangement of all four of them bonded sequentially each to the next. One of the vectors is the bond from from the central atom to one of its attachments. The other two vectors are pairs of the attachments, and thus together represent the plane of the attachments. Improper dihedral angles are useful for analyzing the planarity of the central atom: as the angle deviates from zero, the central atom moves out of the plane defined by the three attached to it.^{[3]}

## Dihedral angles of biological molecules

The backbone dihedral angles of proteins are called φ (*phi*, involving the backbone atoms C'-N-C^{α}-C'), ψ (*psi*, involving the backbone atoms N-C^{α}-C'-N) and ω (*omega*, involving the backbone atoms C^{α}-C'-N-C^{α}). Thus, φ controls the C'-C' distance, ψ controls the N-N distance and ω controls the C^{α}-C^{α} distance.

The planarity of the peptide bond usually restricts ω to be 180° (the typical *trans* case) or 0° (the rare *cis* case). The distance between the C^{α} atoms in the *trans* and *cis* isomers is approximately 3.8 and 2.9 Å, respectively. The *cis* isomer is mainly observed in Xaa-Pro peptide bonds (where Xaa is any amino acid).

The sidechain dihedral angles of proteins are denoted as χ_{1}-χ_{5} for each successive bond along that chain. The χ_{1} dihedral angle is defined by atoms N-C^{α}-C^{β}-C^{γ}, the χ_{2} dihedral angle is defined by atoms C^{α}-C^{β}-C^{γ}-C^{δ}, and so on.

The sidechain dihedral angles tend to cluster near 180°, 60°, and −60°, which are called the *trans*, *gauche ^{+}*, and

*gauche*conformations. The stability of certain sidechain dihedral angles is affected by the neighbouring backbone and sidechain dihedrals; for example, the gauche

^{−}^{+}conformation is rarely followed by the gauche

^{+}conformation (and vice versa) because of the increased likelihood of atomic collisions.

Dihedral angles have also been defined^{[clarification needed]} by the IUPAC for other molecules, such as the nucleic acids (DNA and RNA) and for polysaccharides.

## Methods of computation

The dihedral angle between two planes relies on being able to efficiently generate a normal vector to each of the planes. One approach is to use the cross product. If *A*_{1}, *A*_{2}, and *A*_{3} are three non-collinear points on plane *A*, and *B*_{1}, *B*_{2}, and *B*_{3} are three non-collinear points on plane *B*, then *U*_{A} = (*A*_{2}−*A*_{1}) × (*A*_{3}−*A*_{1}) is orthogonal to plane *A* and *U*_{B} = (*B*_{2}−*B*_{1}) × (*B*_{3}−*B*_{1}) is orthogonal to plane *B*. The (unsigned) dihedral angle can therefore be computed with either

- <math>\varphi_{AB}=\arccos \left(\frac{U_A \cdot U_B}{|U_A| |U_B|}\right) = \arcsin \left(\frac{|U_A \times U_B|}{|U_A| |U_B|}\right)</math>

Another approach to computing the dihedral angle is first to pick an arbitrary vector *V* that is not tangent to either of the two planes. Then applying the Gram–Schmidt process to the three vectors (*A*_{2}−*A*_{1}, *A*_{3}−*A*_{1}, *V*) produces an orthonormal basis of space, the third vector of which will be normal to plane *A*. Doing the same with the vectors (*B*_{2}−*B*_{1}, *B*_{3}−*B*_{1}, *V*) yields a vector normal to plane *B*. The angle between the two normal vectors can then be computed by any method desired. This approach generalizes to higher dimensions, but does not work with flats that have a codimension greater than 1.

To compute the dihedral angle between two flats, it is additionally necessary to ensure that each of the two normal vectors is selected to have a minimal projection onto the other flat. The Gram–Schmidt process does not guarantee this property, but it can be guaranteed with a simple eigenvector technique.^{[4]} If

- <math>\mathbf{A}</math> is a matrix of orthonormal basis vectors for flat
*A*, and - <math>\mathbf{B}</math> is a matrix of orthonormal basis vectors for flat
*B*, and - <math>u \;=</math> the eigenvector with the smallest corresponding eigenvalue of <math>\left(\mathbf{B}^T\mathbf{A}\right)^T\left(\mathbf{B}^T\mathbf{A}\right)</math>, and
- <math>v \;=</math> the eigenvector with the smallest corresponding eigenvalue of <math>\left(\mathbf{A}^T\mathbf{B}\right)^T\left(\mathbf{A}^T\mathbf{B}\right)</math>,

then, the angle between <math>u</math> and <math>v</math> is the dihedral angle between *A* and *B*, even if *A* and *B* have a codimension greater than 1.

## See also

## References

**^**Olshevsky, George,*Dihedral angle*at*Glossary for Hyperspace*.**^**Blondel, Arnaud; Karplus, Martin (7 Dec 1998). "New formulation for derivatives of torsion angles and improper torsion angles in molecular mechanics: Elimination of singularities".*Journal of Computational Chemistry***17**(9): 1132–1141. doi:10.1002/(SICI)1096-987X(19960715)17:9<1132::AID-JCC5>3.0.CO;2-T.**^**CHARMM parmfile.doc definition of "IMPH" energy parameter**^**Gashler, M.; Martinez, T. (2011).*Tangent Space Guided Intelligent Neighbor Finding*(PDF). Proceedings of the IEEE International Joint Conference on Neural Networks (IJCNN'11). pp. 2617–2624.

## External links

- The Dihedral Angle in Woodworking at Tips.FM
- Analysis of the 5 Regular Polyhedra gives a step-by-step derivation of these exact values.
- Weisstein, Eric W., "Dihedral angle",
*MathWorld*.