@explorables/spinwheels/dist/index.es.js

This explorable is a spatial implementation of the Kuramoto Model for phase coupled oscillators. It illustrates spatial synchronization and the dynamics of phase singularities.

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function Zl(t) {
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}
function Xo(t, e) {
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}
function Rn(t, e) {
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}
function Jl(t, e) {
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}
var Wi = 180 / Math.PI, Nr = {
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};
function Bo(t, e, n, r, i, a) {
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var Le;
function Ql(t) {
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function tf(t) {
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function Ho(t, e, n, r) {
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}
var ef = Ho(Ql, "px, ", "px)", "deg)"), nf = Ho(tf, ", ", ")", ")");
function qe(t, e) {
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}
var Wt = 0, fe = 0, se = 0, Uo = 1e3, bn, he, _n = 0, It = 0, jn = 0, we = typeof performance == "object" && performance.now ? performance : Date, Yo = typeof window == "object" && window.requestAnimationFrame ? window.requestAnimationFrame.bind(window) : function(t) {
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};
function Fn() {
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}
function rf() {
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}
function xe() {
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}
xe.prototype = Go.prototype = {
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};
function Go(t, e, n) {
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}
function af() {
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}
function Zi() {
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}
function of() {
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function sf() {
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}
function Tr(t) {
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}
function Ji(t, e, n) {
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}
function uf(t, e, n) {
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}
var cf = No("start", "end", "cancel", "interrupt"), lf = [], Vo = 0, Qi = 1, Sr = 2, en = 3, ta = 4, Pr = 5, nn = 6;
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}
function ui(t, e) {
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}
function it(t, e) {
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}
function J(t, e) {
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function ff(t, e, n) {
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}
function hf(t, e) {
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}
function df(t) {
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}
function pf(t, e) {
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}
function gf(t, e, n) {
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}
function yf(t, e) {
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}
function ci(t, e, n) {
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}
function Ko(t, e) {
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}
function bf(t) {
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}
function _f(t) {
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}
function vf(t, e, n) {
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}
function mf(t, e, n) {
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}
function wf(t, e, n) {
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}
function Mf(t, e) {
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}
function Af(t, e) {
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}
function $f(t, e) {
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}
function Nf(t, e) {
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}
function Tf(t, e) {
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}
function Sf(t, e) {
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}
function Pf(t, e) {
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}
function Ef(t, e) {
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function kf(t) {
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function Of(t, e) {
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}
function zf(t, e) {
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}
function Cf(t) {
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function If(t, e) {
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}
function Rf(t) {
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function jf(t, e) {
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}
function Ff(t) {
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}
function Df(t) {
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}
function Lf(t) {
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}
function qf(t) {
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}
function Xf(t, e, n) {
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}
function Bf(t, e) {
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function Hf(t) {
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}
function Uf() {
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