Unstable vortex: Amplitude
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YouTubeFieldSolver
Unstable vortex: Amplitude
Here we use the complex Ginzburg-Landau equation to model the split of an unstable vortex of n=6 vorticity quanta. We can see that n=6 corresponds to the number of times the phases moves from 0 to 2pi in a full rotation, here invisible due to the amplitude representation chosen We see only a topological defect at the center representing the ...
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Here we use the complex Ginzburg-Landau equation to model the split of an unstable vortex of n=6 vorticity quanta. We can see that n=6 corresponds to the number of times the phases moves from 0 to 2pi in a full rotation, here displayed as a spiral that repeats 6 times. However, any vortex with |n|>1 is unstable, so it must split into stable components, in this case 6 vortices of n=1. These vortices repel each other, distancing and forming an hexagonal grid. The domain is a periodic square of siz
0:20
Here we use the complex Ginzburg-Landau equation to model the split of an unstable vortex of n=6 vorticity quanta. We can see that n=6 corresponds to the number of times the phases moves from 0 to 2pi in a full rotation, here displayed as a spiral that repeats 6 times. However, any vortex with |n|>1 is unstable, so it must split into stable components, in this case 6 vortices of n=1. These vortices repel each other, distancing and forming an hexagonal grid. The domain is a periodic square of siz
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Here we use the complex Ginzburg-Landau equation to model the split of an unstable vortex of n=6 vorticity quanta. We can see that n=6 corresponds to the number of times the phases moves from 0 to 2pi in a full rotation, here displayed as a spiral that repeats 6 times. However, any vortex with |n|>1 is unstable, so it must split into stable components, in this case 6 vortices of n=1. These vortices repel each other, distancing and forming an hexagonal grid. The domain is a periodic square of siz
0:20
Here we use the complex Ginzburg-Landau equation to model the split of an unstable vortex of n=6 vorticity quanta. We can see that n=6 corresponds to the number of times the phases moves from 0 to 2pi in a full rotation, here displayed as a spiral that repeats 6 times. However, any vortex with |n|>1 is unstable, so it must split into stable components, in this case 6 vortices of n=1. These vortices repel each other, distancing and forming an hexagonal grid. The domain is a periodic square of siz
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CS-9 Giza Pyramid & CS-9 Plate!Demonstration of induction ⚡️🚨 and magnetic field vortex 🌀🧬🌪❄️ #pemf
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