Curlingle Notes · Physics

Why curling stones curl — and why physicists still argue about it

A 4-minute read

A curling stone is about as simple as sports equipment gets: a polished disc of granite weighing just under 20 kilograms, with a handle on top. A player slides it down a sheet of ice, giving the handle a gentle twist as they let go. The stone turns slowly, only a few full rotations over its whole trip, and its path bends sideways near the end, in the direction it is spinning. That bend is the "curl" the sport is named after.

Here is the strange part. Turn an empty drinking glass upside down, spin it gently and slide it across a smooth table, and it drifts the other way, against its spin. Intuition built on everyday objects predicts the glass's behaviour, not the stone's. For more than a century, that mismatch has kept physicists busy.

A stone that barely touches the ice

The bottom of a curling stone is not flat. It is concave, so the stone rests only on a narrow ring of rough granite, the running band, roughly the width of a hand across. The ice is not flat either: before a game it is sprayed with fine water droplets that freeze into tiny bumps called pebble. So the stone is a thin ring of rock skating over a field of frozen beads, and the details of that contact turn out to matter enormously.

The glass on the table curls against its spin for a well-understood reason. As it slides, its front edge presses down harder than its back edge, so the front feels more friction. Since the front and back edges are moving sideways in opposite directions because of the spin, the stronger friction at the front wins, and the glass drifts the opposite way. Any explanation for curling has to show why the stone breaks this rule.

Three competing explanations

One family of explanations focuses on friction that changes with speed. The stone's running band may briefly melt a thin film of water as it passes, and friction on ice depends strongly on how fast a surface is sliding over a given spot. If the two sides of the ring experience the ice differently because one side is moving faster over it than the other, the friction becomes lopsided in a way that could push the stone with its spin rather than against it.

A second idea, proposed by researchers at Uppsala University in Sweden, puts the action in scratches. The rough front of the running band scratches the pebbled ice as it passes. Moments later, the back of the band crosses those fresh scratches at an angle, and the grooves steer it, a little like a wheel catching in a rut. Because the back of the stone is guided sideways, the whole stone turns in the direction of its spin.

A third, the "pivot–slide" model developed by physicists in Canada, suggests the stone does not slide smoothly at all. Instead, the running band snags momentarily on individual pebbles at the front, pivots around them, then slides free, thousands of times over a single throw. Each tiny pivot nudges the stone sideways, and the nudges add up to a curl.

A tiny asymmetry repeated thousands of times can bend a path by more than a metre.

The puzzle that won't stay solved

Part of what makes curling hard to explain is that the curl hardly depends on how fast the stone spins. Twist it a little or a lot, and the stone curls by about the same distance. Most simple models predict that more spin should mean more curl, so any successful theory has to explain why the amount of rotation barely matters.

Sweeping adds another layer. When teammates brush the ice in front of a moving stone, they warm and polish the surface, reducing friction. A swept stone travels farther and curls less, which is why sweepers can steer a shot after it has left the thrower's hand. How sweeping interacts with the curl mechanism depends, again, on which theory you believe.

Curling stones have been sliding across frozen lochs in Scotland for roughly five hundred years. The game's rules, equipment and strategy have been refined many times over. Yet the most basic question about it — why does the stone curl? — is still open, a reminder that the physics of everyday contact between two surfaces is far from finished.

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