sherlockjones
- 31
- 0
Lets say we have a vector [tex]\vec{A}(t)[/tex] with a constant magnitude [tex]A[/tex]. Thus [tex]\vec{A}(t)[/tex] can only change in direction (rotation). We know that [tex]\frac{d\vec{A}}{dt}[/tex] is always perpendicular to [tex]\vec{A}[/tex]. This is where I become stuck:
[tex]\Delta \vec{A} = \vec{A}(t+\Delta t)-\vec{A}(t)[/tex]
[tex]|\Delta \vec{A}| = 2A\sin\frac{\Delta \theta}{2}[/tex].
How do we get the trigonometric expression on the right in the second equation? It looks like some type of half/double angle formula. Eventually we are supposed to get [tex]\vec{A}\frac{d\theta}{dt}[/tex] or the angular velocity of [tex]\vec{A}[/tex]
Thanks
[tex]\Delta \vec{A} = \vec{A}(t+\Delta t)-\vec{A}(t)[/tex]
[tex]|\Delta \vec{A}| = 2A\sin\frac{\Delta \theta}{2}[/tex].
How do we get the trigonometric expression on the right in the second equation? It looks like some type of half/double angle formula. Eventually we are supposed to get [tex]\vec{A}\frac{d\theta}{dt}[/tex] or the angular velocity of [tex]\vec{A}[/tex]
Thanks