Here's one way to get different "lines" that satisfy these axioms: you can apply any bijective change of coordinates map.
For instance, apply the coordinate change $x'=x$, $y'=x^2+y$, and then the "lines" of the form $ax' + by' + c = 0$ become $ax + bx^2 + by + c = 0$.
And while the last example was a differentiable change of coordinates with differentiable inverse, one could even apply a discontinuous bijection.
For a different kind of example, one can observe that if $B(\mathcal O,1)$ denotes the open ball of radius $1$ centered at the origin $\mathcal O$, namely
$$B(\mathcal O,1) = \{(x,y) \in \mathbb R^2 \mid x^2 + y^2 < 1\}
$$
then the set of chords in $B(\mathcal O,1)$ satisfies those axioms; by definition a chord is a nonempty subset of $B(\mathcal O,1)$ which can be expressed as the intersection of $B(\mathcal O,1)$ with some straight line $ax+by+c=0$.
If we now choose a bijection $f : B(\mathcal O,1) \to \mathbb R^2$, then we can define a "line" in $\mathbb R^2$ to be the image under $f$ of a chord, and this set of "lines" will satisfy the axioms. For example one can take
$$f(x,y) = (\frac{x}{1-x^2-y^2},\frac{y}{1-x^2-y^2})
$$
This example is fundamentally different from the "standard" example, for instance consider a "triangle" in $B(\mathcal O,1)$ whose vertices are on the boundary circle of $B(\mathcal O,1)$ and hence are not points of the geometry. The three sides of that triangle form three chords $L_1,L_2,L_3$ which do not cross each other, but one of the four components of their complement $B(\mathcal O,1) - (L_1 \cup L_2 \cup L_3)$, namely the interior of the triangle, is incident to each of $L_1,L_2,L_3$. This behavior does not happen with ordinary Euclidean lines.
In fact $B(\mathcal O,1)$ together with its chords form the Beltrami-Klein model of the hyperbolic plane together with its lines. Discovered in the 19th century, this is a model of all of the axioms of Euclidean geometry (hence including Hilbert's incidence axioms) except that it fails to satisfy the parallel postulate.