diff --git a/crates/path/src/ops.rs b/crates/path/src/ops.rs
index 3ad94944d..ba5349312 100644
--- a/crates/path/src/ops.rs
+++ b/crates/path/src/ops.rs
@@ -564,7 +564,8 @@ fn noise(seed: u64, idx: u64, t: f64) -> f64 {
     let i = t.floor();
     let f = t - i;
     let i = i as i64;
-    let p = |k: i64| hash(seed, idx, i + k);
+    // `i` saturates at the i64 ends for an absurd `t`, so the neighbours wrap rather than overflow.
+    let p = |k: i64| hash(seed, idx, i.wrapping_add(k));
     // Catmull-Rom through four lattice values keeps the motion C1-continuous.
     let (p0, p1, p2, p3) = (p(-1), p(0), p(1), p(2));
     let v = 0.5 * (2.0 * p1 + (-p0 + p2) * f + (2.0 * p0 - 5.0 * p1 + 4.0 * p2 - p3) * f * f + (-p0 + 3.0 * p1 - 3.0 * p2 + p3) * f * f * f);
diff --git a/crates/path/src/ops/tests.rs b/crates/path/src/ops/tests.rs
index 89c009bc4..1ebdcea5b 100644
--- a/crates/path/src/ops/tests.rs
+++ b/crates/path/src/ops/tests.rs
@@ -292,6 +292,18 @@ fn wiggle_is_deterministic_and_time_varying() {
     assert_eq!(vertex_count(&a[0]), 4 * 11);
 }
 
+#[test]
+fn wiggle_survives_an_absurd_speed_or_time() {
+    // `t` far past i64 saturates the lattice index at i64::MAX, and the neighbours' `+ 1`, `+ 2` used to overflow.
+    let s = [sq(0.0, 0.0, 100.0)];
+    for v in [f64::INFINITY, f64::NEG_INFINITY, f64::NAN, f64::MAX, f64::MIN, 1e300, 9.3e18] {
+        let by_speed = wiggle(&s, &WiggleParams { speed: v, ..Default::default() }, 1.0);
+        let by_time = wiggle(&s, &WiggleParams::default(), v);
+        let by_phase = wiggle(&s, &WiggleParams { phase_deg: v, ..Default::default() }, 0.0);
+        assert_eq!((by_speed.len(), by_time.len(), by_phase.len()), (1, 1, 1), "wiggle with {v}");
+    }
+}
+
 #[test]
 fn wiggle_displacement_is_bounded() {
     let mut l = BezPath::new();