[itex]\overline{r} (t) = (2t^2)i + (3t - 2)j[/itex]
[itex]convert \ to \ polar \ coordinates \ of \ the \ form \ \overline{r}(t) = \ r \hat{r} \ then \ differentiate![/itex]
1: First we want to calculate |r| = r.
[itex]r \ = \ | \overline{r} | \ = \ \sqrt{(2t^2)^2 + (3t - 2)^2} \ = \sqrt{4t^4 + 9 t^2- 12t + 4}[/itex]
2: We know our unit vector will be;
[itex]\hat{r} \ = \ cos \theta \ + \ \sin \theta[/itex]
3. Calculate θ!
[itex]\theta \ = \ \arctan( \frac{y}{x} ) \ = \ \arctan(\frac{3t - 2}{2t^2} )[/itex]
4. We see that [itex]\hat{r}[/itex] must be;
[itex]\hat{r} \ = \ cos \theta \ + \ \sin \theta \ = \ \cos [\arctan(\frac{3t - 2}{2t^2} )] \ + \ \sin [\arctan(\frac{3t - 2}{2t^2} )][/itex]
5. Put the position vector all together, (all are equivalent).
[itex]\overline{r}(t) = \ r \hat{r}[/itex]
[itex]\overline{r}(t) \ = \ [ \sqrt{4t^4 + 9 t^2- 12t + 4} ] \hat{r}[/itex]
[itex]\overline{r}(t) \ = \ [ \sqrt{4t^4 + 9 t^2- 12t + 4} ] [\ cos \theta \ + \ \sin \theta ][/itex]
[itex]\overline{r}(t) \ = \ ( \sqrt{4t^4 + 9 t^2- 12t + 4} ) (cos \theta ) \ + \ ( \sqrt{4t^4 + 9 t^2- 12t + 4} ) (sin \theta )[/itex]
[itex]\overline{r}(t) \ = \ ( \sqrt{4t^4 + 9 t^2- 12t + 4} ) ( \cos [\arctan(\frac{3t - 2}{2t^2} )] ) \ + \ \sin ( \arctan(\frac{3t - 2}{2t^2} ) ] )[/itex]
[itex]\overline{r}(t) \ = ( \sqrt{4t^4 + 9 t^2- 12t + 4} ) ( \cos [\arctan(\frac{3t - 2}{2t^2} ) ] ) \ + ( \sqrt{4t^4 + 9 t^2- 12t + 4} ) ( \ \sin [\arctan(\frac{3t - 2}{2t^2} ) ] )[/itex]
Alright, so I've set up the position vector as best I can. I'm assuming there's nothing wrong so I'll now take the derivative to find the velocity vector.
6. Using;
[itex]\overline{r}(t) \ = \ [ \sqrt{4t^4 + 9 t^2- 12t + 4} ] [\ cos \theta \ + \ \sin \theta ][/itex]
I'll differentiate to obtain an equation of the form;
[itex]\overline{v} (t) \ = \ \frac{d \overline{r} }{dt} \ = \ r \frac{d \hat{r}}{dt} \ + \ \frac{dr}{dt} \hat{r}[/itex]
Here I go!
[itex]\frac{d \overline{r} }{dt} \ = \ ( \sqrt{4t^4 + 9 t^2- 12t + 4} ) (- sin \theta \frac{d \theta} {dt} \ + \ cos \theta \frac{d \theta}{dt} ) \ + \ ( \frac{16t^3 \ + \ 18t \ - \ 12}{2 \sqrt{4t^4 + \ 9t^2 - 12t + 4} } ) (\ cos \theta \ + \ \sin \theta )[/itex]
[itex]\frac{d \overline{r} }{dt} \ = \ ( \sqrt{4t^4 + 9 t^2- 12t + 4} ) (- sin \theta \ + \ cos \theta ) \frac{d \theta}{dt} \ + \ ( \frac{16t^3 \ + \ 18t \ - \ 12}{2 \sqrt{4t^4 + \ 9t^2 - 12t + 4} } ) (\ cos \theta \ + \ \sin \theta )[/itex]
I didn't dare try to bring in the arctan and it's craziness into this one, (yet...).
7. Look for patterns!
Well,
[itex]r \ = \ \sqrt{4t^4 + 9 t^2- 12t + 4}[/itex]
[itex]\dot{r} \ = \ ( \frac{16t^3 \ + \ 18t \ - \ 12}{2 \sqrt{4t^4 + \ 9t^2 - 12t + 4} } )[/itex]
[itex]\hat{r} \ = \ cos \theta \ + \ \sin \theta[/itex]
[itex]\frac{ d \hat{r}}{dt} \ = \ ( - \sin \theta \ + \ \cos \theta ) \frac{ d \theta}{dt}[/itex]
We'll set;
[itex]\hat{ \theta } \ = \ (- sin \theta \ + \ cos \theta )[/itex]
&
[itex]\dot{ \theta} \ = \ \frac{d \theta}{dt}[/itex]
to get
[itex]\frac{ d \hat{r}}{dt} \ = \ \hat{ \theta } \dot{ \theta}[/itex]
8. Write the final, simplified equation for velocity.
[itex]\overline{v} (t) \ = \ r \dot{ \theta} \hat{ \theta } \ + \ \dot{r} \hat{r}[/itex]
Comparing the result of 8. with the result of 6. using 7. to be sure we've labelled everything correctly I'd say we have taken a deceptively simple equation in cartesian form, converted it to it's equivalent polar coordinate description & take the derivative of this to obtain the velocity.
Q.E.D.
[tex]\alpha :[/tex]Have I missed anything?
[tex]\beta :[/tex] Have you ever actually had to do a calculation like this??