Thanks for the update bob. I'm not even sure that it's true that you might see more of a reflection from a flatter element, but reckon it's not the case that you'd see it more due to the distance - it's a bit more involved than that.
That the curvature creates a flare is actually an interesting little problem for ray optics. I might have a play with it over the weekend - it's not something for a weeknight for me!
we are talking about different things here
the reflectivity of a material is dependant of the refractive index of the material, and the medium it is in. As we are talking air, lets look at crown glass n = 1.523
The thinner lenses (higher refractive index) are more shiny. Plastics materials in common use vary from 1.4 - 1.7 and glass n=1.5 - n=1.8 (1.9 is very rare)
As R=((n1-n2)/(n1+n2))^2 we end up with
0.533/2.523^2 = 5.3% reflection from each surface of the lens. The curvature of the lens is irrelevant
Nowadays we have lenses with multiple anti reflective coatings that bring the reflectivity of each surface down to 0.1% and better. They achieve this by phase cancelling the reflection
The thing with filters is that they:
1. have no MAR or just a single layer AR coating, so are more reflective
2. often are not light sealed to the lens, allowing incident light in "round the back)
it is irrelevant where the surface is, if it is light-sealed. if you were in a blacked out studio, with a single window at the other end, you would see no reflection from the INSIDE of the window, as the room is blacked out and there is no light directly striking the inside surface of the window from within the room. This is pretty much the case for most lens elements IN a lens system (camera, telescope, binoculars, microscope etc.)
The only spanner in the works is that you can have internal reflections within a lens, however the power of these are very small, as to see one at the sensor, it has to have been reflected at least twice, and remember, for crown glass, we are talking 5% is reflected, 95 % transmitted at each surface