Question #73681

For a particle undergoing circular motion with an angular velocity w in in a circle of radius r show that
w×(w×r) = -w^2.r

Expert's answer

Answer on Question #73681 – Math – Vector Calculus

QUESTION

For a particle undergoing circular motion with an angular velocity ω\vec{\omega} in a circle of radius rr show that


ω×(ω×r)=ω2r\vec{\omega} \times (\vec{\omega} \times \vec{r}) = -\omega^2 \vec{r}


SOLUTION

To solve this problem, we need to recall some formulas and facts:

1) The formula for the vector triple product (from a linear algebra)


a×(b×c)=b(ac)c(ab),\vec{a} \times (\vec{b} \times \vec{c}) = \vec{b}(\vec{a} \cdot \vec{c}) - \vec{c}(\vec{a} \cdot \vec{b}),


where


ac=accos(φ) is the scalar (dot) product of vectors\vec{a} \cdot \vec{c} = |\vec{a}| \cdot |\vec{c}| \cdot \cos(\varphi) \text{ is the scalar (dot) product of vectors}aa=aacos(0)=aa=a2\vec{a} \cdot \vec{a} = |\vec{a}| \cdot |\vec{a}| \cdot \cos(0{}^\circ) = a \cdot a = a^2


(More information: https://en.wikipedia.org/wiki/Triple_product)

(More information: https://en.wikipedia.org/wiki/Dot_product)

2) An angular velocity


ωrωr=ωrcos(90)=ωr0=0\vec{\omega} \perp \vec{r} \rightarrow \vec{\omega} \cdot \vec{r} = |\vec{\omega}| \cdot |\vec{r}| \cdot \cos(90{}^\circ) = |\vec{\omega}| \cdot |\vec{r}| \cdot 0 = 0ωrωr=0\boxed{\vec{\omega} \perp \vec{r} \rightarrow \vec{\omega} \cdot \vec{r} = 0}


(More information: https://en.wikipedia.org/wiki/Angular_velocity)

In our case,


ω×(ω×r)=ω(ωr)r(ωω)=ω0rω2=ω2r\vec{\omega} \times (\vec{\omega} \times \vec{r}) = \vec{\omega}(\vec{\omega} \cdot \vec{r}) - \vec{r}(\vec{\omega} \cdot \vec{\omega}) = \vec{\omega} \cdot 0 - \vec{r} \cdot \omega^2 = -\omega^2 \vec{r}


Thus,


ω×(ω×r)=ω2r\boxed {\vec {\omega} \times (\vec {\omega} \times \vec {r}) = - \omega^ {2} \vec {r}}


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