Not a full answer, but possibly the start of one. I came across a paper[1] discussing some mathematical properties of fullerene graphs. In section 4.2, they give a formula for a lower bound on the diameter based on the number of vertices $n$, assuming there are only pentagonal and hexagonal face.
$$\text{diam}(F)\ge\frac{\sqrt{24n-15}}{6}-\frac{1}{2}$$
Given a lower bound on the diameter, it may be possible to prove that a ball of a certain size would be mechanically unstable. I suspect this would give a fairly high upper bound on the size and it wouldn't account for the wide variety of shapes that are possible for fullerenes[2], but this would at least be a starting point.
This could hopefully be refined somewhat by using the largest synthesized/reported fullerene size as a lower bound. Thus far $\ce{C_{500}}$ is the largest fullerene I can find experimental evidence for [3,4]. I suspect this is still pretty far from the largest possible fullerene, even considering just spherical/icosahedral structures.
Based on [2], you will need to look for some kind of mechanical/kinetic stability limit for the upper bound, as the paper suggests that fullerenes should increase in thermodynamic stability as $n$ increases, approaching the structure of graphene or a infinite nanotube.
- Vesna Andova, František Kardoš, Riste Škrekovski. Mathematical aspects of fullerenes. Ars Mathematica Contemporanea, DMFA Slovenije, 2016, 11, pp.353 - 379. ffhal-01416354f
- WIREs Comput Mol Sci 2015, 5:96–145. doi: 10.1002/wcms.1207
- Shinohara, H., Sato, H., Saito, Y., Izuoka, A., Sugawara, T., Ito, H., Sakurai, T. and Matsuo, T. (1992), Extraction and mass spectroscopic characterization of giant fullerences up to C500. Rapid Commun. Mass Spectrom., 6: 413-416. https://doi.org/10.1002/rcm.1290060702
- Front. Chem., 03 December 2020 | https://doi.org/10.3389/fchem.2020.607712