User contributions for Rosso
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1 March 2024
- 19:5919:59, 1 March 2024 diff hist +1 L-6 →Dynamics
- 19:5719:57, 1 March 2024 diff hist +336 L-6 →Critical Force
- 19:3319:33, 1 March 2024 diff hist +19 L-6 →Critical Force
- 19:2919:29, 1 March 2024 diff hist +471 L-6 →Stationary solution
29 February 2024
- 18:4118:41, 29 February 2024 diff hist +5 L-6 →Dynamics
- 18:4018:40, 29 February 2024 diff hist +19 L-6 →Dynamics
- 18:3818:38, 29 February 2024 diff hist +36 L-6 →Stationary solution
- 18:0818:08, 29 February 2024 diff hist −6 L-6 →Dynamics
- 18:0618:06, 29 February 2024 diff hist +63 L-6 →Dynamics
- 17:5817:58, 29 February 2024 diff hist −819 L-6 →Dynamics
- 17:5217:52, 29 February 2024 diff hist +1,163 L-6 →Fully connected (mean field) model for the cellular automaton
- 15:5115:51, 29 February 2024 diff hist +2 L-6 →Fully connected (mean field) model for the cellular automaton
- 15:5015:50, 29 February 2024 diff hist +316 L-6 →Fully connected model foor the cellular automata (mean field)
- 15:0915:09, 29 February 2024 diff hist +239 L-6 →Avalanches and BGW process
28 February 2024
- 23:3523:35, 28 February 2024 diff hist +2,602 N L-6 Created page with "= Avalanches and BGW process= = Fully connected model foor the cellular automata (mean field)= Let's study the mean field version of the cellular automata introduced in the previous lecture. * The elastic coupling is with all neighbours <center><math> \sigma_i= h_{CM} - h_i + m^2(w-h_i), \quad </math></center>. * The local random threshold are all equal: <center> <math> \sigma_i^{th}=1, \quad \forall i </math></center>. Instead of following the evoluion..."
- 23:2923:29, 28 February 2024 diff hist −2,168 L-5 →Cellular Automata
- 23:1823:18, 28 February 2024 diff hist +1 L-5 →Cellular Automata
- 22:4922:49, 28 February 2024 diff hist +1,298 L-5 →Cellular Automata
- 18:0518:05, 28 February 2024 diff hist −232 L-5 →Scaling behaviour of the depinning transition
- 18:0018:00, 28 February 2024 diff hist +204 L-5 →Equation of motion
26 February 2024
- 11:5311:53, 26 February 2024 diff hist +6 L-5 →Stationary solution
- 11:5311:53, 26 February 2024 diff hist +7 L-5 →Stationary solution
- 11:5211:52, 26 February 2024 diff hist +500 L-5 →Fully connected model (mean field)
- 10:5710:57, 26 February 2024 diff hist +166 L-5 →Fully connected model (mean field)
25 February 2024
- 20:2720:27, 25 February 2024 diff hist +7 L-5 →Fully connected model (mean field)
- 20:2420:24, 25 February 2024 diff hist +14 L-5 →Fully connected model (mean field)
- 20:2320:23, 25 February 2024 diff hist −104 L-5 →Fully connected model (mean field)
- 20:2120:21, 25 February 2024 diff hist +6 L-5 →Fully connected model (mean field)
- 20:2020:20, 25 February 2024 diff hist +304 L-5 →Fully connected model (mean field)
- 20:1320:13, 25 February 2024 diff hist +2 L-5 →Fully connected model (mean field)
- 20:1220:12, 25 February 2024 diff hist +253 L-5 →Cellular Automata
- 18:5118:51, 25 February 2024 diff hist +138 L-5 →Cellular Automata
- 18:1118:11, 25 February 2024 diff hist +1 L-5 →Cellular Automata
- 18:1018:10, 25 February 2024 diff hist +368 L-5 →Cellular Automata
- 17:5717:57, 25 February 2024 diff hist +326 L-5 →Fully connected model (mean field)
- 17:4317:43, 25 February 2024 diff hist +99 L-5 →Cellular Automata
- 16:5516:55, 25 February 2024 diff hist +23 L-5 →Cellular Automata
- 14:1214:12, 25 February 2024 diff hist +371 L-5 →Cellular Automata
21 February 2024
- 20:5820:58, 21 February 2024 diff hist +472 L-5 →Cellular Automata
- 20:3620:36, 21 February 2024 diff hist +242 L-5 →Cellular Automata
- 20:2320:23, 21 February 2024 diff hist +424 L-5 →Cellular Automata
- 20:0720:07, 21 February 2024 diff hist +185 L-5 →Scaling behaviour of the depinning transition
- 20:0320:03, 21 February 2024 diff hist −1 L-5 →Equation of motion
- 20:0320:03, 21 February 2024 diff hist +136 L-5 →Scaling behaviour of the depinning transition
- 19:1019:10, 21 February 2024 diff hist +142 L-5 →Scaling behaviour of the depinning transition
- 19:0519:05, 21 February 2024 diff hist +158 L-5 →Scaling behaviour of the depinning transition
- 18:5818:58, 21 February 2024 diff hist +242 L-5 →Scaling behaviour of the depinning transition
- 18:2118:21, 21 February 2024 diff hist +586 L-5 →Scaling behaviour of the depinning transition
- 17:5717:57, 21 February 2024 diff hist +962 L-5 →Equation of motion
- 12:3112:31, 21 February 2024 diff hist −3 L-5 →Equation of motion