| MadSci Network: Physics |
Man, that was some question you asked. I thought about it for a long time and then wound up asking a lot of people who didn't know either. This answer comes to you courtesy of my friend Dean McLaughlin, a postdoc in Astronomy at Berkeley. One thing that's important for the soap film is that it's thin, relative to the wavelength of the light passing through it. If a plane mirror is much thicker than one wavelength (as it obviously is), then the angular separation between consecutive interference minima and maxima will be something like (this is probably wrong, but you get the idea): sin(theta_max) - sin(theta_min) = lambda/2d where d is the thickness of the mirror glass. If that's even 1 cm, then for visible lambda=550 nm, it looks to me like the minima and maxima are separated by only 0.00003 rad. At the same time, large angles theta_max for an individual fringe are obtained only for the highest orders, which are way down in intensity. So while the effect has to be there, maybe the answer is just that it's unobservable in the plane-mirror case. (The canonical soap film has d comparable to lambda.) Thanks again for your question.
Try the links in the MadSci Library for more information on Physics.