A particle moves along the ellipse $3x^2 + y^2 = 1$ with positions vector $\vec{r(t)} = f(t)\vec i + g(t) \vec j$. The motion is such that the horizontal component of the velocity vector at time $t$ is $-g(t)$. How much time is required for the particle to go once around the ellipse?
Now I found that the particle travels counterclockwise, though I suspect it doesn't matter. I also found that the position vector is $(x, ±\sqrt{1-3x^2} )$ and hence the velocity vector is $(\mp \sqrt{1-3x^2} , 3x)$.
I am not supposed to use arc length, so I am quite confused as to how to solve this problem. I am guessing that I am supposed to integrate something, but what, how, and why....
Lets paremertize the elipse
$f(t) = \frac {1}{\sqrt 3}\cos (\omega(t))\\ g(t) = \sin (\omega (t))$
and it is given that: $f'(t) = -g(t)$
$f'(t) = -(\frac {1}{\sqrt 3}\cos \omega)\omega' = \sin (\omega (t))\\ \omega' = \sqrt 3\\ \omega(t) = \sqrt 3 \ t$
It will take $\frac {2\pi}{\sqrt 3}$ to complete one orbit.
Or you could say
$(x,y) = (\omega(t), \sqrt {1-3\omega^2})$
But this only gets you half way around.... then you need to get back along the path
$(x,y) = (\omega(t), -\sqrt {1-3\omega^2})$
$\omega' = -\sqrt {1-3\omega^2}$
and we solve the differential equation and get the same trig equations we have above.