4 ms·
I wonder if there are materials of one-way reflectance so that all of the sphere would be used instead of a particular face. Why would this be used over a phas
by adolph 3y ago
I wonder if there are materials of one-way reflectance so that all of the sphere would be used instead of a particular face.
Why would this be used over a phased array where the paraboloid shape is created in software post-processing?
- mikewarot 3y agoIt's not the sphere that does the work, it's the parabola inside it, cutting it in half.
- ben_w 3y agoOne-way reflectance isn't a really real thing in physics, the closest you get is the illusion from having a bright room and a dark room on opposite sides of a mostly-reflective boundary. https://en.wikipedia.org/wiki/One-way_mirror https://en.wikipedia.org/wiki/One-way_mirror
- nomel 3y agoIf you give me a polarized wave, I can give you a surface that reflects in one direction, and passes in the other, with awful efficiency. ;)
- itishappy 3y agoIt wouldn't help. Focusing requires a concave surface, and the inside of the sphere is the only concave bit. Coating the outside would create an omnidirectional reflector, but it'd be super low-gain. We actually tried exactly this with Project Echo. https://en.wikipedia.org/wiki/Project_Echo https://en.wikipedia.org/wiki/Project_Echo Also, "one-way reflectance" is largely a myth. One-way mirrors in police stations and stores are actually just partially reflective mirrors with a dark room on one side. A true one-way reflector would involve an optical circulator, which tends to be a small, sensitive, expensive component, not something you can coat over a flexible surface. https://en.wikipedia.org/wiki/Optical_circulator https://en.wikipedia.org/wiki/Optical_circulator Lastly, the main advantage is cost and simplicity. Phased arrays use fancy semiconductors. This gives you a lot of features and benefits, but comes at significant cost. This antenna is more or less a Mylar party balloon, it would not surprised me if it's orders of magnitudes cheaper.