An aeroplane in steady level flight is an equilibrium with wings: lift equals weight, and thrust equals drag. This lesson works that balance against the curves from the previous lesson to answer three questions the syllabus asks again and again: between which speeds can the aeroplane fly level, what happens when the balance is disturbed, and at what speed does staying airborne cost the least fuel?
The equilibrium of level flight
In straight and level flight at a steady speed, the thrust exactly matches the drag, which is why the drag curve is also called the thrust-required curve. Both drag and power required follow their bucket shapes against speed: high at the slow end (induced drag dominating), high again at the fast end (parasite drag dominating), cheapest in the middle. Now disturb the balance. If the thrust set exceeds the drag at the current speed, the surplus is excess thrust, and with the pilot holding altitude it accelerates the aeroplane; the speed rises, the drag rises with it, and the acceleration ends when drag has grown to meet the thrust again. Set less thrust than drag and the same logic runs backwards, and the power picture tells the same story: power available above power required accelerates the aeroplane at constant altitude until the required power catches up. Level flight at a steady speed is always a meeting point of the two curves.
Reading the curves
Draw the thrust-available line across the thrust-required bucket and the geometry answers the speed-envelope question directly. The curves cross twice: the left intersection is the minimum speed for level flight that thrust can sustain, and the right intersection is the maximum speed for level flight. Between them the available line sits above the bucket, and the gap is excess thrust available for accelerating or climbing; outside them level flight cannot be held. In practice the stall usually intervenes before the thrust-limited minimum is reached, so the left intersection is more theory than technique; the right one is very real.