Why is the special orthogonal group considered the rotation group?

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SUMMARY

The special orthogonal group, denoted as SO(3), consists of orthogonal matrices that satisfy the conditions x·x^T=I and det(x)=1. These matrices represent pure rotations in three-dimensional space, preserving both the dot products of vectors and the orientation of a right-handed basis. The determinant of a rotation operator must be 1 to ensure that it does not dilate or shrink any volume, distinguishing it from reflections which have a determinant of -1. Understanding these properties is crucial for grasping the mathematical foundations of rotation in linear algebra.

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  • Understanding of linear algebra concepts, specifically orthogonal matrices
  • Familiarity with determinants and their geometric interpretations
  • Knowledge of the special orthogonal group SO(3) and its properties
  • Basic understanding of vector dot products and their preservation under transformations
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tensor33
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I understand that the special orthogonal group consists of matrices x such that x\cdot x=I and detx=1 where I is the identity matrix and det x means the determinant of x. I get why the matrices following the rule x\cdot x=I are matrices involved with rotations because they preserve the dot products of vectors. The part I don't get is why the matrices involved with rotation must have determinant 1.
 
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A pure rotation should not dilate or shrink any volume. The determinant of a linear operator is the scale factor by which the volume element increases. Hence, the determinant of a rotation operator must be 1.
 
tensor33 said:
I understand that the special orthogonal group consists of matrices x such that x\cdot x=I and detx=1 where I is the identity matrix and det x means the determinant of x. I get why the matrices following the rule x\cdot x=I are matrices involved with rotations because they preserve the dot products of vectors. The part I don't get is why the matrices involved with rotation must have determinant 1.

Did you mean x\cdot x^T=I??

Muphrid said:
A pure rotation should not dilate or shrink any volume. The determinant of a linear operator is the scale factor by which the volume element increases. Hence, the determinant of a rotation operator must be 1.

That doesn't really explain why the determinant can't be -1, which is what the OP is asking.
The reason is that rotations preserves the orientation of a basis. If we have a right-handed basis, then rotations of this will be right-handed as well.
As an example of an orthogonal matrix that does not preserve the orientation, you can probably take a reflection.
 
tensor33 said:
I understand that the special orthogonal group consists of matrices x such that x\cdot x=I and detx=1 where I is the identity matrix and det x means the determinant of x. I get why the matrices following the rule x\cdot x=I are matrices involved with rotations because they preserve the dot products of vectors. The part I don't get is why the matrices involved with rotation must have determinant 1.
To prove that rotations have determinant 1, you must first define the term "rotation". It's perfectly OK to just take "R is said to be a rotation if R is a member of SO(3)" as the definition, but then there's nothing to prove. Another option is "R is said to be a rotation if R is a member of the largest connected subgroup of O(3)". Then your task would be to prove that the largest connected subgroup is SO(3).

(I actually prefer the terminology that calls members of O(3) rotations, and members of SO(3) proper rotations).
 
micromass said:
Did you mean x\cdot x^T=I??

Ya, I forgot the transpose part.

Thanks to all those who replied, I'm pretty sure I get it now.
 

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