Archive for the '–' Category
Stanley Milgram – Wikipedia, the free encyclopedia
November 1, 2015Small-world experiment – Wikipedia, the free encyclopedia
November 1, 2015Belousov–Zhabotinsky reaction – Wikipedia, the free encyclopedia
November 1, 2015Arthur Winfree – Wikipedia, the free encyclopedia
November 1, 2015THE INFAMOUS “SQUIDGYGATE” TRANSCRIPT
November 1, 2015pecora : “may I have the phone number for colonel y, I cannot confirm” or deny – Google Search
November 1, 2015QT:{{”
Once Pecora asked himself whether chaos could be useful. playful physicist with a ….. May I have the phone number for Colonel Y?” “I cannot confirm or deny that anyone … “I cannot confirm or deny that he works here. isn’t it?
“}}
Phys. Rev. Lett. 71, 65 (1993) – Circuit implementation of synchronized chaos with applications to communications
November 1, 2015Sending Your Secrets Safely with Chaos | Logical Tightrope
November 1, 2015QT:{{”
Cuomo’s method relies on this synchronized chaos, a somewhat mysterious discovery summarized in a 1990 paper [2] by Louis Pecora and Thomas Carroll at The Naval Research Laboratory. The phenomenon occurs in some situations when part of the outputof one chaotic system is used as an input for a twin chaotic system. If the two systems are properly synchronized, then the second system will mimic the behavior of the first with uncanny fidelity.
Just like Pecora, Carroll, Cuomo, and Oppenheim have done, we’ll look at synchronization in the chaotic Lorenz system (look at my post Edward Lorenz’s Strange Attraction for a Deeper Dive into the Lorenz system). The system comes from Edward Lorenz’s simplification of an atmospheric convection model, and its intriguing chaotic behavior has been studied for decades. It is defined by the following system of nonlinear differential equations:
“}}
http://logicaltightrope.com/2013/09/01/sending-your-secrets-safely-with-chaos/
Attractor – Wikipedia, the free encyclopedia
November 1, 2015QT:{{”
A trajectory of the dynamical system in the attractor does not have to satisfy any special constraints except for remaining on the attractor, forward in time. The trajectory may be periodic or chaotic. If a set of points is periodic or chaotic, but the flow in the neighborhood is away from the set, the set is not an attractor, but instead is called arepeller (or repellor).
“}}
