Math 2.0

Mechanics of particles and systems Definition

Euler angles

Builds on Special orthogonal groupRotation

Definition

For θ∈ℝ\theta \in \R, let Rz(θ)=(cos⁡θ−sin⁡θ0sin⁡θcos⁡θ0001),Rx(θ)=(1000cos⁡θ−sin⁡θ0sin⁡θcos⁡θ)R_z(\theta) = \begin{pmatrix} \cos\theta & -\sin\theta & 0 \\ \sin\theta & \cos\theta & 0 \\ 0 & 0 & 1 \end{pmatrix}, \qquad R_x(\theta) = \begin{pmatrix} 1 & 0 & 0 \\ 0 & \cos\theta & -\sin\theta \\ 0 & \sin\theta & \cos\theta \end{pmatrix} be the rotations of ℝ3\R^3 by the angle θ\theta about the zz-axis and the xx-axis. Let RR be an element of the special orthogonal group SO(3)SO(3). A triple (α,β,γ)(\alpha, \beta, \gamma) of real numbers is a triple of Euler angles of RR, in the zz-xx-zz convention, if:

  1. α∈[0,2π)\alpha \in [0, 2\pi), β∈[0,π]\beta \in [0, \pi] and γ∈[0,2π)\gamma \in [0, 2\pi);
  2. R=Rz(α) Rx(β) Rz(γ)R = R_z(\alpha)\, R_x(\beta)\, R_z(\gamma).

Remarks

Every R∈SO(3)R \in SO(3) has a triple of Euler angles, and the triple is unique when 0<β<π0 < \beta < \pi. The angle β\beta is determined by cos⁡β=R33\cos\beta = R_{33}, the entry in the third row and third column.

Example: the triple (π/2,0,0)(\pi/2, 0, 0) gives R=Rz(π/2)R = R_z(\pi/2), the quarter turn about the zz-axis. But (0,0,π/2)(0, 0, \pi/2) and (π/4,0,π/4)(\pi/4, 0, \pi/4) give the same RR, since Rx(0)R_x(0) is the identity; at β=0\beta = 0 only α+γ\alpha + \gamma is determined (gimbal lock).

Non-example: the product Rz(α)Rz(β)Rz(γ)=Rz(α+β+γ)R_z(\alpha) R_z(\beta) R_z(\gamma) = R_z(\alpha + \beta + \gamma) is not of the form in clause 2. Such products only give rotations about the zz-axis, so three rotations about one axis cannot serve as Euler angles.

Other conventions use other axis sequences. Proper Euler angles have equal first and third axes, such as zz-yy-zz. Tait–Bryan angles use three distinct axes, such as yaw, pitch and roll about zz, yy, xx. The product Rz(α)Rx(β)Rz(γ)R_z(\alpha) R_x(\beta) R_z(\gamma) can be read as rotations about the fixed axes in the order γ\gamma, β\beta, α\alpha. It can also be read as rotations about the moving body axes in the order α\alpha, β\beta, γ\gamma.

Reading path

To understand this page from the ground up, read these 16 pages in order. The foundations come first.

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Each page uses the pages above it. The colour of the bar on a box shows how strong the evidence is, and the box also gives it as text. The list has the same pages.
  • no evidence level
  1. Euclidean isometry concept
  2. Euclidean plane object
  3. Identity matrix object
  4. Matrix definition
  5. Vector space definition
  6. Rotation definition
  7. Square matrix definition
  8. Transpose definition
  9. Linear map definition
  10. Orthogonal matrix definition
  11. Multilinear map definition
  12. Orthogonal group object
  13. Alternating multilinear map definition
  14. Determinant definition
  15. Special orthogonal group object
  16. Euler angles definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Euler_angles
About this page
TagYRSV2AASVB
URIm2://YRSV2AASVB
Kinddefinition
WritingW0 stub
MSC70B10, 15B10
DefinesEuler angles
UsesSpecial orthogonal group, Rotation
Changed3 November 2026

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