I’m sorry that nobody else has given you an answer here. I’ll try, but there’s a good chance that anybody else would have given a better than what you see below. The little algebraic geometry I learned, I learned in an earlier geological era, so my treatment will be laughably old-fashioned.
Let’s try to use Riemann-Roch. Let’s call the constant field $\kappa$, and the hyperelliptic function field, $K$. Let’s choose one Weierstrass point, and label it $I$, it’s going to be special. You know that there’s one new element of the function field $K$ with a double pole at $I$, let’s call it $\xi\in K$, and $\xi^2$ has pole of order four at $I$. Genus two implies that there’s a new function with pole of order $5$ at $I$, call it $\eta$, which is not in the $\kappa$-span of $\{1,\xi,\xi^2\}$. From there on, for every order of pole $6\le n\le9$, there’s a new function with pole of order $n$, they’re $\xi^3$, $\eta\xi$, $\xi^4$, and $\eta\xi^2$, respectively. But with pole of order ten, there are two new functions, $\xi^5$ and $\eta^2$, so there must be a $\kappa$-linear relation
$$
b\eta^2+a_1\eta\xi^2+a_3\eta\xi+a_5\eta
=c\xi^5+a_2\xi^4+a_4\xi^3+a_6\xi^2+a_8\xi+a_{10}\,,
$$
where $bc\ne0$, that is, $\eta^2$ and $\xi^5$ definitely must appear in the relation of linear dependence. It’s an old story, but by choosing $\lambda_1,\lambda_3,\lambda_5$ correctly, you can set $\eta=\eta'+\lambda_1\xi^2+\lambda_3\xi+\lambda_5$, still in the same linear space, still with a pole of order $5$ at $I$, so that $b{\eta'}^2=c\xi^5+a'_2\xi^4+a'_4\xi^3+a'_6\xi^2+a'_8\xi+a'_{10}\,$. In other words, we have
$$
{\eta'}^2=\mu\prod_{i=1}^5(\xi-\rho_i)\,,\quad\rho_i\in\kappa, \mu\in\kappa^\times
$$
at least if $\kappa$ is algebraically closed (and you can treat the general case very easily). Let’s call $Q(\xi)$ that quintic polynomial in $\xi$, for convenience.
Now, in this model of your curve, the hyperelliptic involution acts on a point $(\alpha,\beta)$ to change the sign of $\beta$, and the five other Weierstrass points are $P_i=(\rho_i,0)$, and we can call $I=P_6$. At this point, since the divisor of $\xi-\rho_i$ is $2P_i-2I$, you see why $P_i-P_j$ gives a point of order two on the Jacobian, and for the fact about the “two remaining points”, that comes from the fact that
the divisor of $\eta'$ is $-5I+\sum_1^5P_i$.