LondonLady
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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
\displaystyle{\frac{d\theta}{dt} = \omega}
Now assume that the circle has radius r and that
\displaystyle{\frac{d\theta}{dt} = 2t}
for t in seconds. Let \theta(t = 0) = 0
(therefore \theta = t^2)
a) Find \vec{r}(t)
b) Find \vec{v}(t). is \vec{v} \perp \vec{r}?
c) Find \vec{a}(t). Express \vec{a} in terms of \vec{r} and \vec{v}. Is \vec{a} \perp \vec{v}?
d) With respect to the circle's centre, sketch \vec{r},\vec{v} and \vec{a} 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 \vec{r} \perp \vec{v} and that \vec{a} \perp \vec{v}. I have also found that \vec{a} can be written as -\alpha \vec{r} (where \alpha is a constant. All this implies that the acceleration vector is pointed back into the centre of the circle as some negative multiple of \vec{r}.
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
\displaystyle{\frac{d\theta}{dt} = \omega}
Now assume that the circle has radius r and that
\displaystyle{\frac{d\theta}{dt} = 2t}
for t in seconds. Let \theta(t = 0) = 0
(therefore \theta = t^2)
a) Find \vec{r}(t)
b) Find \vec{v}(t). is \vec{v} \perp \vec{r}?
c) Find \vec{a}(t). Express \vec{a} in terms of \vec{r} and \vec{v}. Is \vec{a} \perp \vec{v}?
d) With respect to the circle's centre, sketch \vec{r},\vec{v} and \vec{a} 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 \vec{r} \perp \vec{v} and that \vec{a} \perp \vec{v}. I have also found that \vec{a} can be written as -\alpha \vec{r} (where \alpha is a constant. All this implies that the acceleration vector is pointed back into the centre of the circle as some negative multiple of \vec{r}.
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?