How to Calculate a 3x3 Rotation Matrix around a Given Axis?

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To calculate a 3x3 rotation matrix for a rotation of Pi/6 around the axis defined by the vector (1, 2, 3), first clarify the rotation direction, which is suggested to be clockwise. The rotation matrix can be derived by determining the effects of the rotation on the standard basis vectors [0,0,1], [0,1,0], and [1,0,0]. After computing these results, constructing the matrix becomes straightforward. Additional resources, such as Wikipedia and MathWorld, may provide further guidance on rotation matrices. Understanding these steps is essential for successfully calculating the desired rotation matrix.
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Hi, if i want to find a 3x3 matrix R which represents a rotation of Pi/6 around the axis of rotation v(vector)={1, 2, 3}. how can i find it?
 
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Are you saying that your axis is along a vector that starts at the origin of the coordinate system and has its tip at the point (x,y,z)=(1,2,3)? And is your rotation direction clockwise or counterclockwise as viewed from the perspective of (0,0,0)?
 
Originally posted by Janitor
Are you saying that your axis is along a vector that starts at the origin of the coordinate system and has its tip at the point (x,y,z)=(1,2,3)? And is your rotation direction clockwise or counterclockwise as viewed from the perspective of (0,0,0)?
Thanks. it's a vector from origin to (1, 2, 3). which direction? i am not sure yet. let say clockwise.
 
Start by figuring out what the result of rotating
[0,0,1]
[0,1,0]
and
[1,0,0]
are.

Once you've done that, you shouldn't have any trouble making hte matrix.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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