Esta lección aún no está traducida. Por ahora se muestra en inglés; la versión en español está en camino.
A polar curve $r = f(\theta)$ is really a parametric curve with $\theta$ as the parameter. Once you write it that way, slopes and lengths come straight from the parametric formulas, and they pair well with polar area.
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Write $x = r\cos\theta$ and $y = r\sin\theta$ with $r = f(\theta)$. The product rule gives
$$\frac{dx}{d\theta} = r'\cos\theta - r\sin\theta,$$ $$\frac{dy}{d\theta} = r'\sin\theta + r\cos\theta.$$
Squaring and adding, the cross terms $\pm 2rr'\sin\theta\cos\theta$ cancel and $\sin^{2} + \cos^{2} = 1$, leaving
$$\left(\frac{dx}{d\theta}\right)^{2} + \left(\frac{dy}{d\theta}\right)^{2} = r^{2} + (r')^{2}.$$
That makes sense: as $\theta$ changes, the point moves out along the ray at rate $r'$ and around the circle at rate $r$, two directions at right angles.
The cardioid $r = 1 + \cos\theta$ drawn as $x = r\cos\theta$, $y = r\sin\theta$. The arrow is the velocity in $\theta$, and the readout adds up the length so far. Slide to $\theta = 2\pi$: the total length is 8.
So the integrand is $2\left|\cos\frac{\theta}{2}\right|$. By symmetry, double the length for $0 \le \theta \le \pi$, where $\cos\frac{\theta}{2} \ge 0$.
Using the Cartesian formula $\int\sqrt{1 + (r')^{2}}\,d\theta$. Test on the circle $r = 3$ for $0 \le \theta \le 2\pi$, whose length is $6\pi$: the correct integrand is $\sqrt{9 + 0} = 3$, giving $6\pi$; the wrong one gives $\sqrt{1} = 1$ and only $2\pi$. In polar form the "1" is replaced by $r^{2}$, because moving around a circle of radius $r$ covers distance $r\,\Delta\theta$, not $\Delta\theta$.
At the origin ($r = 0$) the slope formula simplifies to $\frac{dy}{dx} = \tan\theta$: the curve leaves the pole along the ray at that angle. For the rose $r = \cos 3\theta$, the petals touch the pole along $\theta = \pm\frac{\pi}{6}$, $\frac{\pi}{2}$.
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