Position vector in spherical coordinates.

AI Thread Summary
The discussion revolves around determining the position vector of point P on a rotating wheel in spherical coordinates. The wheel, with radius R, rotates in the xy-plane about the z-axis with an angular velocity described by Ct². The initial position of point P is given as P(0, R, 0), which translates to spherical coordinates as P(R, π/2, π/2). The main challenge lies in correctly expressing the time-dependent term for the azimuthal angle φ, as it changes with time due to the wheel's acceleration. The user seeks clarification on how to incorporate the angular velocity into the position vector while recognizing that the motion is more complex than a simple integration of angular velocity.
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I have not done this in a while and I am having a brain fart.

Given: A wheel of radius R rotates with angular velocity Ct2 k\hat{} (lies in x-y plane, rotating about z). A point P on the circles is P(x,y,z) = (0,R,0)

Ques: What is the position vector of point P in spherical coordinates?

Ans: Now I know that P(x,y,z) -> P(r,\theta,\phi,) = (R, \pi/2,\pi/2)

I want to say P(r,\theta,\phi,) = R \hat{r} + \{pi/2}\hat{\theta} + \{pi/2}\hat{\phi}, but that tells me P never moves. Considering P is on a spinning disk, it must some how correlate to Ct2 \hat{k}


Maybe I'm just overlooking this. Can some one point me in the right direction?
 
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sorry, having coding issues.
 
any ideas
 
Last edited:
I cleaned up the presentation a bit, hopefully to make it a bit easier for those that can share some advice.

Given: A wheel of radius R rotates with an angular velocity. The wheel lies in the xy plane, rotating about the z-axis.

P(x,y,z) = (0,R,0)

\overrightarrow{\omega}= Ct^2\hat{k}

Ques: What is the position vector of point P in spherical coordinates?

Ans: Now I know that,

P(r,\theta,\phi,) = (R,\frac{\pi}{2},\frac{\pi}{2})

But I don't think that helps much.

For the position vector, I can't figure out the term for:

\hat{\phi}

I have:

\overrightarrow{r}= R\ \hat{r}+\frac{\pi}{2}\ \hat{\theta}+\ \ \ \ \ \ \ \ \hat{\phi}

The last term is giving me issues.
 
Now I know that \phi changes with time, so the term must depends on t.

I also know that \omega is rad/s, which can also be interpreted as \phi/s.

But I don't think it is legal to just integrate \omega to get position. Is it?

Since the angular velocity is quadratic, that means the disc is accelerating. So the position should be third order correct?

I'm being really stubborn here because I know it is something minute that is keeping me from progressing.
 
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