Let the position of a particle in three dimensional space at time t be $(t, \cos t, \sin t)$. Then the length of the path traversed by the particle between the times $t = 0$ and $t = 2\pi$ is
(A) $2\pi$.
(B) $2\sqrt{2}\pi$
(C) $\sqrt{2}\pi$
(D) none of the above.
My thoughts: $ds = \sqrt{(dx)^2 + (dy)^2 + (dz)^2}dt=\sqrt{(1 + \sin^2t + \cos^2t)} dt$ = $\sqrt{2} dt$
Integrating between $t = 0$ and $t = 2\pi$, I get $2\sqrt{2}\pi$.
However, If I try to visualise this :
$\cos^2t +\sin^2t = 1$. so, $x^2+y^2 =1$
Hence, the particle describes a circle in yz plane. and in xy plane it is a cosine wave, in xz plane it is a sine wave. combining these three, it seems that for each $2\pi$ time it completes one revolution in xy plane. Each revolution is the perimeter of the circle $x^2+y^2 =1$, so it should be $2\pi$.
I am getting conflicting answers.
I am not sure if I have done this correctly. Can someone help me confirm this ?
Thanks.


By definition, the arc-length of a curve $\gamma: [a,b] \to \Bbb R^n$ is: $$L[\gamma] = \int_a^b \|\gamma'(t)\|\,{\rm d}t.$$ Here, $\gamma: [0,2\pi] \to \Bbb R^3$ is given by $\gamma(t) = (t,\cos t, \sin t)$, so $\gamma'(t) = (1,-\sin t, \cos t)$ and so: $$\|\gamma'(t)\| = \sqrt{2} \implies L[\gamma] = \int_0^{2\pi}\sqrt{2}\,{\rm dt} = 2\sqrt{2} \pi.$$
It is not $2\pi$. The vertical displacement adds a bit of length there. Not even the $x^2+y^2=1$ circle, actually.. it would be the $y^2+z^2=1$. And if you think in $3D$, these equations by themselves describe cylinders, not circles.