How do vectors relate to perpendicularity in circular motion?

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Homework Help Overview

The discussion revolves around the relationship between vectors in circular motion, specifically focusing on the position, velocity, and acceleration vectors, as well as their perpendicularity. The context involves a mathematical exploration of circular motion with a time-dependent angular velocity.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the mathematical relationships between the position vector, velocity vector, and acceleration vector in circular motion. Questions arise regarding the implications of perpendicularity and the behavior of the particle as it speeds up.

Discussion Status

Some participants have provided insights into the differentiation of vectors and the conditions for perpendicularity. There is an ongoing exploration of the implications of these relationships, with no explicit consensus reached on the interpretations of the acceleration vector's direction.

Contextual Notes

Participants are navigating the complexities of time-dependent angular velocity and its effects on the vectors involved in circular motion. There is a noted confusion regarding the acceleration vector's relationship to the velocity vector and the implications for the motion of the particle.

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

[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?
 
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The position vector is perpendicular to the velocity vector, but the acceleration vector is NOT perpendicular to the velocity vector!
 
hmm... thankyou for your reply. I can't agree though. I got

[tex]\vec{r}(t) = r\cos (t^2)\vec{i} + r\sin (t^2)\vec{j}[/tex]

[tex]\vec{v}(t) = -2tr\sin (t^2)\vec{i} + 2tr\cos (t^2)\vec{j}[/tex]

[tex]\vec{a}(t) = -4t^2r\cos(t^2)\vec{i} - 4t^2r\sin(t^2)\vec{j}[/tex]

Then if you find the dot product

[tex]\vec{a}.\vec{v} = 8t^3r^2\sin(t^2)\cos(t^2) - 8t^3r^2\sin(t^2)\cos(t^2) = 0[/tex]

Which implies they are perpendicular... Is my logic wrong?
 
You have not differentiated [tex]\vec{v}[/tex] correctly:
[tex]\frac{d\vec{v}}{dt}=(\frac{d}{dt}2tr)(-\sin(t^{2})\vec{i}+\cos(t^{2})\vec{j})+2tr\frac{d}{dt}(-\sin(t^{2})\vec{i}+\cos(t^{2})\vec{j})=[/tex]
[tex]2r(-\sin(t^{2})\vec{i}+\cos(t^{2})\vec{j})+4t^{2}r(-\cos(t^{2})\vec{i}-\sin(t^{2})\vec{j})[/tex]
 
Ahh! It didnt even occur to me that it might have changed into a product! Thankyou so much!
 

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