MHB Understanding Velocity and Acceleration of a Moving Particle

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The position vector of a particle is defined as $\vec{r}=\cos{(\omega t)}\hat{i} + \sin{(\omega t)}\hat{j}$. To determine the velocity $\vec{v}$, differentiate the position vector with respect to time, yielding $\vec{v}$. The discussion emphasizes that if the dot product $\vec{r} \cdot \vec{v} = 0$, then the vectors are perpendicular. Additionally, the cross product $\vec{r} \times \vec{v}$ is shown to be a constant vector. Understanding these concepts requires knowledge of calculus and vector operations.
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A particle moves so that its position vector is given by $\vec{r}=\cos{(\omega t)}\hat{i} + \sin{(\omega t)}\hat{j}$. Show that the velocity $\vec{v}$ of the particle is perpendicular to $\vec{r}$ and $\vec{r} \times \vec{v}$ is a constant vector.

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First calculate [math]\vec{v} = \dfrac{d \vec{r}}{dt}[/math]. If [math]\vec{r} \cdot \vec{v} = 0[/math] for all t then they are always perpendicular.

-Dan
 
Since the velocity function is the derivative of the position function and the acceleration function is the derivative of the velocity function, I would say, "start by taking a Calculus class!". Have you done that? Do you know what the derivatives of $cos(\omega t)$ and $sin(\omega t)$ are? Do you know how to show that one vector is perpendicular to another? (Dot product.)
 
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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