Yes, I do believe there is and that is the approach I outline in my answer to the Physics SE equation "What's so special about the speed of light" as well as my answer here. I like to think of SR as simply Galileo's basic idea but with the assumption of absolute time relaxed (not to devalue Einstein's bold step in making this relaxation).

One begins with the first relativity postulate in the common approach (actually I like to refer here to the poetic allegory of Salviati's ship by Galileo). One then splits it into about three more precise axioms: the (1) first postulate together with assumptions of (2) homogeneity of space and time and (3) symmetry of the relationships between two inertial observers, one deduces linearity of the transformation. These assumptions show that the coordinate transformation must indeed be affine - so there you have your affine space straight away. JoshPhysics does this here (his answer to Physics SE "Homogeneity of space implies linearity of Lorentz transformations") and Mark H does it beautifully here (his answer to "Why do we write the lengths in the following way? Question about Lorentz transformation".

All of the above + absolute time implies precisely Galileo's relativity and that the Galilean group is the unique group of transformations possible. Relax absolute time, and the Galilean group becomes just one of a member of a family of possible groups, which are all Lorentz groups with different values of $c$.

I applaud your approach, because the "what's so special about the speed of light" or "what's light got to do with it anyway" (SR) is something that drives many teenage scientists batty. When I first heard about relativity at ten years old, that question drove me to distraction. And I have been asked it by people of that age more times than I can count in my 51 years. When I was 15, I had read all about Maxwell's equations and thought I knew the answer: I knew roughly Einstein's first approach to the problem. I therefore had the impression that SR is ALL ABOUT light and that light is very special. There's nothing wrong with seeing the first approach to this problem. But you do not need light to explain SR and in your proposed approach it turns things around and says "hey, we found an experimental example of something that transforms with a finite $c$ Lorentz transformation. So what does SR then say about this thing?". In other words, we use SR to study and understand light, not the other way around. I simply think that an approach like yours is a more fundamental, simpler and pedagogically better. I don't think Einstein would have minded in the least that our approach to teaching SR should move on after 110 years!

Your proposed approach seems to have been first thought about by Vladimir Ignatowsky around 1911.

A truly offbeat and original approach was raised in the comments to the Physics SE question "Why is spacetime not Riemannian?". Scifi author Greg Egan motivates the signature of pseudometric very well in his "Orthogonal", where he studies what the world would be like with a Euclidean signature.

Yes, I do believe there is and that is the approach I outline in my answer to the Physics SE equation "What's so special about the speed of light" as well as my answer here. I like to think of SR as simply Galileo's basic idea but with the assumption of absolute time relaxed (not to devalue Einstein's bold step in making this relaxation).

One begins with the first relativity postulate in the common approach (actually I like to refer here to the poetic allegory of Salviati's ship by Galileo). One then splits it into about three more precise axioms: the (1) first postulate together with assumptions of (2) homogeneity of space and time and (3) symmetry of the relationships between two inertial observers, one deduces linearity of the transformation. These assumptions show that the coordinate transformation must indeed be affine - so there you have your affine space straight away. JoshPhysics does this here (his answer to Physics SE "Homogeneity of space implies linearity of Lorentz transformations") and Mark H does it beautifully here (his answer to "Why do we write the lengths in the following way? Question about Lorentz transformation".

All of the above + absolute time implies precisely Galileo's relativity and that the Galilean group is the unique group of transformations possible. Relax absolute time, and the Galilean group becomes just one of a member of a family of possible groups, which are all Lorentz groups with different values of $c$.

I applaud your approach, because the "what's so special about the speed of light" or "what's light got to do with it anyway" (SR) is something that drives many teenage scientists batty. When I first heard about relativity at ten years old, that question drove me to distraction. And I have been asked it by people of that age more times than I can count in my 51 years. When I was 15, I had read all about Maxwell's equations and thought I knew the answer: I knew roughly Einstein's first approach to the problem. I therefore had the impression that SR is ALL ABOUT light and that light is very special. There's nothing wrong with seeing the first approach to this problem. But you do not need light to explain SR and in your proposed approach it turns things around and says "hey, we found an experimental example of something that transforms with a finite $c$ Lorentz transformation. So what does SR then say about this thing?". In other words, we use SR to study and understand light, not the other way around. I simply think that an approach like yours is a more fundamental, simpler and pedagogically better. I don't think Einstein would have minded in the least that our approach to teaching SR should move on after 110 years!

Your proposed approach seems to have been first thought about by Vladimir Ignatowsky around 1911.

A truly offbeat and original approach was raised in the comments to the Physics SE question "Why is spacetime not Riemannian?". Scifi author Greg Egan motivates the signature of pseudometric very well in his "Orthogonal", where he studies what the world would be like with a Euclidean signature.