Speed to fly is √((a + Mc) / c)
A quadratic sink polar w(V) = a + b V + c V² (sink positive) and a next-thermal climb Mc satisfy the classic MacCready condition w + Mc = V w′. The linear term cancels, and the speed to fly is Vstf = √((a + Mc)/c). With Mc = 0 that is also the still-air best-glide speed, √(a/c). Minimum sink, when the polar has a useful linear term, is at −b/(2c). A polar w = 1 + 0.0025 V² (knots of airspeed and sink) and a 3-knot MacCready setting therefore fly at 40 knots, with 5 knots of sink; still-air best glide is 20 knots on that same (intentionally simple) polar.
A real glider polar is measured, not invented, and speed to fly also changes in sinking or rising air between thermals and with a headwind or tailwind (a cruise-speed addition this page does not apply). Use the polar from the flight manual or a logger, not a guess. Related tools: glide distance and the drag polar / L/D max calculator.
Sources
- P. B. MacCready, “Optimum Airspeed Selector,” Soaring, 1958.
- FAA Glider Flying Handbook, speed to fly and MacCready theory.
- Helmut Reichmann, Cross-Country Soaring (quadratic polar and speed-to-fly).
Frequently asked questions
What MacCready setting should I use?
The expected climb rate in the next thermal, in the same units as sink. Mc = 0 is still-air best glide — useful when you only need to reach a point, not to average a high cross-country speed.
Why does the linear coefficient disappear?
The MacCready condition is w + Mc = V dw/dV. For a quadratic, that reduces to a + Mc = c V², independent of b. Minimum-sink speed still depends on b.
Does this include wind?
No. A headwind raises the speed to fly and a tailwind lowers it. This page is the still-air MacCready speed.