Beginner's question about homotopy type in Milnor's Morse Theory

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In the introductory section of Milnor's Morse Theory, he gives an example of the torus.

Diagram 1 from Morse Theory by John Milnor

The set of points of the torus which have height less than $a$ for some $p<a<q$ is just a solid disk, i.e., a 2-cell. When we move from $q$ to $r$, we start getting a cylinder. Milnor notes that moving from a 2-cell to a cylinder is the same (homotopically) as attaching a 1-cell:

Image from Morse Theory by John Milnor

I can sort of understand why: A cylinder can be squashed into a circle, and the bottom half of the left side is homotopically a point, so both sides are homotopically the same as a circle.

But at the same time, moving from $q$ to $r$ means attaching something which looks kind of like the pair of pants:

enter image description here

We can squash the legs together to get a circle, so doesn't this mean that we are attaching a circle to our disk, instead of just a line?

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A pair of pants doesn't have the same homotopy type as a circle. You can flatten it and then contract it to the shape of the digit 8, i.e. two circles glued at a point. pair of pants contracting to figure 8 In any case, who says that the cancellation law holds when gluing topological spaces together? You know that $$\text{disk} + \text{pair of pants} \approx \text{disk} + \text{line.}$$ Why should you expect that $$\text{pair of pants} \approx \text{line?}$$