Answer on Question #73681 – Math – Vector Calculus
QUESTION
For a particle undergoing circular motion with an angular velocity ω ⃗ \vec{\omega} ω in a circle of radius r r r show that
ω ⃗ × ( ω ⃗ × r ⃗ ) = − ω 2 r ⃗ \vec{\omega} \times (\vec{\omega} \times \vec{r}) = -\omega^2 \vec{r} ω × ( ω × r ) = − ω 2 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 ⃗ ( a ⃗ ⋅ c ⃗ ) − c ⃗ ( a ⃗ ⋅ b ⃗ ) , \vec{a} \times (\vec{b} \times \vec{c}) = \vec{b}(\vec{a} \cdot \vec{c}) - \vec{c}(\vec{a} \cdot \vec{b}), a × ( b × c ) = b ( a ⋅ c ) − c ( a ⋅ b ) ,
where
a ⃗ ⋅ c ⃗ = ∣ a ⃗ ∣ ⋅ ∣ c ⃗ ∣ ⋅ cos ( 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} a ⋅ c = ∣ a ∣ ⋅ ∣ c ∣ ⋅ cos ( φ ) is the scalar (dot) product of vectors a ⃗ ⋅ a ⃗ = ∣ a ⃗ ∣ ⋅ ∣ a ⃗ ∣ ⋅ cos ( 0 ∘ ) = a ⋅ a = a 2 \vec{a} \cdot \vec{a} = |\vec{a}| \cdot |\vec{a}| \cdot \cos(0{}^\circ) = a \cdot a = a^2 a ⋅ a = ∣ a ∣ ⋅ ∣ a ∣ ⋅ cos ( 0 ∘ ) = a ⋅ 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
ω ⃗ ⊥ r ⃗ → ω ⃗ ⋅ r ⃗ = ∣ ω ⃗ ∣ ⋅ ∣ r ⃗ ∣ ⋅ cos ( 90 ∘ ) = ∣ ω ⃗ ∣ ⋅ ∣ r ⃗ ∣ ⋅ 0 = 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 = 0 ω ⊥ r → ω ⋅ r = ∣ ω ∣ ⋅ ∣ r ∣ ⋅ cos ( 90 ∘ ) = ∣ ω ∣ ⋅ ∣ r ∣ ⋅ 0 = 0 ω ⃗ ⊥ r ⃗ → ω ⃗ ⋅ r ⃗ = 0 \boxed{\vec{\omega} \perp \vec{r} \rightarrow \vec{\omega} \cdot \vec{r} = 0} ω ⊥ r → ω ⋅ r = 0
(More information: https://en.wikipedia.org/wiki/Angular_velocity)
In our case,
ω ⃗ × ( ω ⃗ × r ⃗ ) = ω ⃗ ( ω ⃗ ⋅ r ⃗ ) − r ⃗ ( ω ⃗ ⋅ ω ⃗ ) = ω ⃗ ⋅ 0 − r ⃗ ⋅ ω 2 = − ω 2 r ⃗ \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} ω × ( ω × r ) = ω ( ω ⋅ r ) − r ( ω ⋅ ω ) = ω ⋅ 0 − r ⋅ ω 2 = − ω 2 r
Thus,
ω ⃗ × ( ω ⃗ × r ⃗ ) = − ω 2 r ⃗ \boxed {\vec {\omega} \times (\vec {\omega} \times \vec {r}) = - \omega^ {2} \vec {r}} ω × ( ω × r ) = − ω 2 r
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