The polar, and what MacCready does to it

Speed to fly is one tangent line drawn on one curve. Almost nobody sees it drawn — it arrives as a number from a flight computer, or as a rule of thumb about pushing forward in sink. Drag the handle below and watch the line move.

Speed polar

min sink best glide

Drag the dark handle — it is the point the tangent is drawn from, at (headwind, minus your MacCready setting). That is the whole construction.

Speed to fly

Sink at that speed

Glide at that speed

Achieved XC speed

Best glide

Minimum sink

Density ratio σ

Beyond the published data for this polar. The curve was fitted over a narrower speed range, so this answer is an extrapolation — and a quadratic under-predicts sink at high speed, which means the number is optimistic. Treat it as indicative and add margin.

Conditions

MacCready is the average climb you expect in the next thermal, as your averager will read it. Not the netto reading, not what the last one gave you.

Polar is at . Ballast never changes best glide — only the speed you achieve it at.

A published polar is a sea-level curve. Both axes scale by 1/√σ with altitude — work out yours.

Your glider's polar

We do not ship a database of gliders, and the reason is on the page below. Put your own aircraft's published figures in — it takes about thirty seconds with the flight manual open.

A standard-class glass ship at 33 kg/m², near enough an LS 4 — a teaching curve, not a claim about any particular aircraft. Best glide 39.8 at 96 km/h, minimum sink 0.60 m/s at 75 km/h. Use it to see how the construction behaves, then put your own numbers in.

Every flight manual prints these. Three of them fix the curve completely; the fourth is then a check, not an input.

Those three speeds imply a best glide of , against the :1 you entered — .

A gap this size means the published numbers are not mutually consistent with a quadratic polar. That is common, and it is usually the headline glide ratio that is the optimistic one. The curve here is built from the two speeds and the sink rate, because those are measurements; the glide ratio is a conclusion.

The limitation to keep in mind: both of those points are slow ones, and speed to fly is always faster than best glide. So every speed-to-fly answer from this mode is an extrapolation past the last number you gave it. If your manual has a polar graph, use the three-point mode with one fast point and this problem goes away.

Read three points off the polar graph in your flight manual. Make one of them fast — that is what fixes the high-speed end, which is the end speed-to-fly actually lives at.

Sink positive: 1.05 means descending at 1.05. The fitted range becomes your slowest to your fastest point, and the curve is dashed outside it.

The wing loading the published polar was measured at — printed next to the graph in most manuals. Your own all-up wing loading goes in Conditions above.

The numbers behind the curve
Glide ratio

Greyed rows are outside the fitted range.

What this assumes, and what it can't know

This is ground school, not a flight computer. It exists to make the geometry visible — where the tangent touches, what moves when the wind changes, why ballast does not improve your glide ratio. Fly the aircraft and the instruments in front of you.

We ship no glider database, deliberately, and here is the arithmetic behind that. Given minimum sink and best-glide speed, the best glide ratio is determined — it is not a free number. Take the Standard Discus's own published figures, 0.59 m/s at 78 km/h and best glide at 100 km/h: they imply 41.9, against a published 45. A 7% gap, with no way to know which of the three numbers is wrong. Shipping that as "the Discus polar" would mean publishing a curve that contradicts its own source, so we ask you for your manual's numbers instead — the same reason the cockpit load tool asks you to read the placard.

A quadratic is a fit, not the physics. Outside the range it was fitted over it fails in one direction: it under-predicts sink at high speed, because real drag rise outruns a parabola, and below minimum-sink speed it knows nothing about the stall. Both errors flatter the glider, which is the dangerous direction, so extrapolated segments are dashed and extrapolated answers are flagged.

The bugs slider is crude and optimistic. One multiplier on the whole curve leaves best-glide speed unchanged, whereas real contamination raises profile drag and would lower it. So the modelled speed to fly is faster than reality and any height requirement derived from it is too low. It also ignores that rain raises your stall speed. Add margin.

Glide ratio here is through the air. Over the ground it is better with a tailwind and worse with a headwind, which is exactly what the tangent construction is showing you when you move the wind.

Not yet reviewed by anyone but us. If you run a club's books and one of these assumptions is wrong, we would genuinely rather hear it than not — tell us and we'll credit you here. This is a budgeting estimate, not a quote. Every club sets its own rates and they change; check with the club before relying on a number.

What the polar will not tell you

Ballast leaves your glide ratio untouched and shifts the whole curve to higher speed, so on this page water always looks free. It is not: it costs you climb, and the climb penalty is the entire reason there is a decision to make. That trade-off is not on this chart.

Read: what a polar actually tells you →