# Decomposition of 3D rotation (in analogy to translation)

Any displacement along a line can be written as the sum of two perpendicular displacements, which then form a closed triangle with the total displacement vector.

My question is: Can something similar be done with rotation?

Consider a rotation about a fixed axis. Can this always be decomposed into two rotations about two perpendicular axes, which again form a triangle (or similar) with the total axis of rotation? In other words, if the axis of rotation is inclined such that it has components in $$x$$ and $$y$$ with respect to a global coordinate system, will the rotation it permits never involve a rotation about the $$z$$-axis?

If it is indeed possible to consider rotations in this way, what is the simplest way to decompose the rotation into fractional contributions from these two putative axes?

EDIT (in response to comment):

A "sharpened" version of my "theorem" may read as: Any rotation about a fixed arbitrary axis can be decomposed into a rotation about three orthogonal axes, but not into a rotation about two orthogonal axes."

• Linked. Be mindful you need three , not two, Euler angles. Commented Mar 15, 2023 at 14:37
• The wording of your "never involve" proposed theorem is worded ambiguously. Can you sharpen it as a "true or false" such? The axis of rotation of any great circle on the globe can be arrived at by unique longitude and latitude rotations. Commented Mar 15, 2023 at 14:45
• @CosmasZachos do we need three angles for rotation about a fixed axis? Commented Mar 15, 2023 at 15:35
• No he is not! That's why I asked him to parse out his "theorem"... What could you imagine my point to be? He obviously needs to review the Gibbs composition formula. Commented Mar 15, 2023 at 16:02
• What do you mean by rotations? Becasue for infinitesimal rotations, or for rotational speeds yes you can decompose the vector into two components, but for finite rotations the answer is not exactly. Commented Mar 15, 2023 at 17:11

You are probably asking about the Gibbs composition of rotations (1884), an idiosyncratic non-abelian law. If you describe a rotation by a Gibbs vector $$\mathbf{g} = \hat{\mathbf{e}}\tan\frac{\theta}{2},$$ where $$\hat{\mathbf{e}}$$ is the unit direction of the rotation and $$\theta$$ the rotation angle, then the Gibbs vector of two such successive rotations g and f is $$(\mathbf{g},\mathbf{f}) = \frac{\mathbf{g}+\mathbf{f}-\mathbf{f}\times\mathbf{g}}{1-\mathbf{g}\cdot\mathbf{f}} \,.$$