I'm reading a textbook on differential geometry and the author proceeds to define a weaker version of homotopy.
Two continuous curves $c_0, c_1: [a,b] \to U \subseteq \mathbb{R}^n$ with the same endpoints are homotopic if there exists a continuous map $H: [a,b] \times [0,1] \to U$ such that $H(s,0) = c_0(s), H(s,1)=c_1(s)$ and $H(a,t) = c_0(a), H(b,t) = c_0(b).$ If the last condition is dropped, we say $H$ is a free homotopy.
A proof of line integral invariance under homotopy proceeds and at the end the author says
If $c_0, c_1$ are closed curves ($c_0(a) = c_0(b), c_1(a) = c_1(b)$) that are freely homotopic, then $H(a,t), H(b,t)$ are equal curves.
This is equivalent to every curve in the free homotopy being closed, but I don't see why this has to be true. In fact, why can't we slightly open a loop and then shrink it to a point? There has to be some continuity problem with what I'm imagining since in the case of a simple loop around the origin, this contradicts the fact that $\mathbb{R}^2 \setminus \{0\}$ is not simply connected. In fact, I didn't even think about this issue until reading through the book caused me to imagine it.
The continuity issue must be very subtle since the partial derivatives (with respect to $s, t$) exist and are continuous in the example of slightly opening a loop. I suspect that letting $(s,t)$ approach $(a, 0)$ from different directions will seal the deal. With that in mind, how do I go back and prove $c_t(s) = H(s,t)$ is a closed curve for all $t$?
Update: The book is Differential Forms and Applications by Do Carmo. In fact, the author defines simple-connectedness as every closed curve being freely homotopic to a point and says $\mathbb{R}^2 - \{0\}$ is not simply connected later, so my example better not work. But now I've changed my mind and am starting to think it works again.
Let $C_t$ be the unit circle with the top half dilated to have radius $1+t$ and center at $(t,0).$ Consider a free homotopy from $C_0$ to $C_1$ back to $C_0.$ We must already have a violation of continuity at $t=0$ else after getting to $C_{\epsilon},$ we can just shrink to a point. The exact equation for $H : [0, 2\pi] \times [0,1] \to \mathbb{R}^2$ is $H(s,t) = (t + (1+t)\cos s, (1+t)\sin s)$ when $s \le \pi$ and this is clearly a continuous function of $s, t.$ Thus, $H$ is continuous on $A = [0, \pi] \times [0,1], B = [\pi, 2\pi] \times [0,1], A \cap B = \{\pi\} \times [0,1],$ so is continuous on the whole domain $A \cup B.$