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mvg:lecture_03:start [2018/11/29 13:44] – [Comments] adminmvg:lecture_03:start [2018/11/29 14:21] – [TRansformation between Lie Algebra and Lie Group] admin
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 $\dot{R}R^T = - (R\dot{R^T})^T$, is skew symmetric! $\dot{R}R^T = - (R\dot{R^T})^T$, is skew symmetric!
  
-$\dot{R}R^T = \hat{w} \Leftrightarrow \dot{R}= \hat{w}R(t)$ +$\dot{R}R^T = \hat{w} \Leftrightarrow \dot{R}(t)= \hat{w}R(t)$  
 + 
 +$R(dr) = R(0) + dR = I + \hat{w}(0)dt$ 
 + 
 +==== TRansformation between Lie Algebra and Lie Group ==== 
 + 
 +Lie Algebra: $so(3) = \{\hat{w} | w \in \mathbb{R}^3\}$ of skew symmetric matrices 
 + 
 +Lie Group: $SO(3)$, smooth manifold and a group 
 + 
 +The Lie algebra $so(3)$ is the tangent space at the identity of the rotation group $SO(3)$ 
 + 
 +algebra over a field K is a vector space over K with multiplication on the space V. Not commutative. 
 + 
 +Lie Brackets: 
 + 
 +$\left[\hat{w},\hat{v}\right] \identical \hat{w}\hat{v}-\hat{v}\hat{w} \in so(3)$ 
 + 
 +Two Lie groups we will study: $so(3), se(3)$  
 + 
 +=== Exponential Map === 
 + 
 +$\left{ \dot{R}(t)=\hat{w}R(t) \right. $ 
 + 
 +$R(0) = I$ 
 + 
 +How does the rotation matrix change from one time within a little time step? 
 + 
 + 
 +$R(t) = e^{\hat{w}t} = \sum ...$ expansion. That solves the diff. eqn. above. 
 + 
 +$\exp: so(3) \rightarrow SO(3)\quad \hat{w} -> e^{\hat{w}}$ 
 +   
  
mvg/lecture_03/start.txt · Last modified: 2018/12/23 18:45 by admin