- #1
LondonLady
- 14
- 0
Im a bit confused about a question on circular motion that I'm answering. Ill state the entire question and then say what I am confused about.
In class we discussed circular motion for the case
[tex]\displaystyle{\frac{d\theta}{dt} = \omega}[/tex]
Now assume that the circle has radius [tex]r[/tex] and that
[tex]\displaystyle{\frac{d\theta}{dt} = 2t}[/tex]
for [tex]t[/tex] in seconds. Let [tex]\theta(t = 0) = 0[/tex]
(therefore [tex]\theta = t^2[/tex])
a) Find [tex]\vec{r}(t)[/tex]
b) Find [tex]\vec{v}(t)[/tex]. is [tex]\vec{v} \perp \vec{r}[/tex]?
c) Find [tex]\vec{a}(t)[/tex]. Express [tex]\vec{a}[/tex] in terms of [tex]\vec{r}[/tex] and [tex]\vec{v}[/tex]. Is [tex]\vec{a} \perp \vec{v}[/tex]?
d) With respect to the circle's centre, sketch [tex]\vec{r},\vec{v}[/tex] and [tex]\vec{a}[/tex] for counter clockwise rotation.
Ok. I have found all the vectors in i-j form. My question is about the perpendicularity questions. Mathematically I have found that [tex]\vec{r} \perp \vec{v}[/tex] and that [tex]\vec{a} \perp \vec{v}[/tex]. I have also found that [tex]\vec{a}[/tex] can be written as [tex]-\alpha \vec{r}[/tex] (where [tex]\alpha[/tex] is a constant. All this implies that the acceleration vector is pointed back into the centre of the circle as some negative multiple of [tex]\vec{r}[/tex].
If this is so then how is the particle speeding up?? (the rate of change of theta is time dependent)
I would have thought that the acceleration vector would have been at some angle to the position vector. But then it wouldn't move in a circle... I am confused...
Also, the second part of (c) I am finding hard. Anyone any ideas?
In class we discussed circular motion for the case
[tex]\displaystyle{\frac{d\theta}{dt} = \omega}[/tex]
Now assume that the circle has radius [tex]r[/tex] and that
[tex]\displaystyle{\frac{d\theta}{dt} = 2t}[/tex]
for [tex]t[/tex] in seconds. Let [tex]\theta(t = 0) = 0[/tex]
(therefore [tex]\theta = t^2[/tex])
a) Find [tex]\vec{r}(t)[/tex]
b) Find [tex]\vec{v}(t)[/tex]. is [tex]\vec{v} \perp \vec{r}[/tex]?
c) Find [tex]\vec{a}(t)[/tex]. Express [tex]\vec{a}[/tex] in terms of [tex]\vec{r}[/tex] and [tex]\vec{v}[/tex]. Is [tex]\vec{a} \perp \vec{v}[/tex]?
d) With respect to the circle's centre, sketch [tex]\vec{r},\vec{v}[/tex] and [tex]\vec{a}[/tex] for counter clockwise rotation.
Ok. I have found all the vectors in i-j form. My question is about the perpendicularity questions. Mathematically I have found that [tex]\vec{r} \perp \vec{v}[/tex] and that [tex]\vec{a} \perp \vec{v}[/tex]. I have also found that [tex]\vec{a}[/tex] can be written as [tex]-\alpha \vec{r}[/tex] (where [tex]\alpha[/tex] is a constant. All this implies that the acceleration vector is pointed back into the centre of the circle as some negative multiple of [tex]\vec{r}[/tex].
If this is so then how is the particle speeding up?? (the rate of change of theta is time dependent)
I would have thought that the acceleration vector would have been at some angle to the position vector. But then it wouldn't move in a circle... I am confused...
Also, the second part of (c) I am finding hard. Anyone any ideas?