Private Pilot · Unit 2 · 20 min

Left-Turning Tendencies

Lesson goals

By the end of this lesson you will know:

Why the nose pulls left

Push the throttle in for takeoff and the airplane tries to yaw left. Hold it straight down the runway and you find your right foot already pressing the pedal. That left yaw is not one effect but four, each produced by the spinning propeller, and all four are strongest in exactly the regime a new pilot first meets them: high power, high angle of attack, and low airspeed, which is the takeoff and initial climb. This lesson takes them one at a time, because the knowledge test asks you to name and distinguish them, and then shows how they combine in the cockpit.

One convention governs everything that follows. On nearly every American single-engine airplane, the propeller turns clockwise as seen from the pilot's seat, looking forward. Every direction stated below assumes that rotation. An airplane whose propeller turns the other way, as some foreign designs do, has its tendencies reversed, but the trainer you fly turns clockwise, so its tendencies pull the nose left.

PHAK Ch 5, "Torque and P-Factor"

The propeller is a rotating wing

Before the four tendencies make sense, one fact about the propeller has to be in place. Each blade is an airfoil, the same kind of curved cross-section as the wing, and as it spins it meets the air at an angle of attack and produces an aerodynamic force. On the wing that force is lift, acting upward. On a propeller blade the force tilts forward, and its forward component is thrust. The wing lesson, How a Wing Generates Lift, established that an airfoil's force grows with the angle at which it meets the relative wind and with the speed of the air past it. Both facts drive the tendencies below: torque and slipstream follow from the blades producing force at all, and P-factor follows from the two sides of the disc meeting the air at different angles.

That is as far as this lesson needs to go into the propeller. How the blade angle is built in, why the blade is twisted from hub to tip, and how fixed-pitch and constant-speed propellers differ are taken up in the Unit 3 lesson The Engine and Propeller. Here it is enough to treat each blade as a small rotating wing making a forward force.

PHAK Ch 5, "Propeller Principles"

Torque reaction

Airframe reaction (rolls left) Propeller (action) Right wing rises Left wing drops
Torque reaction, seen head-on, so the airplane's left wing is on your right. The propeller turns clockwise from the cockpit, so by Newton's third law the airframe rolls the opposite way: a left roll about the longitudinal axis that drops the left wing and raises the right. Airplane drawing by Werneuchen (Wikimedia Commons, public domain).

Newton's third law states that for every action there is an equal and opposite reaction. The engine turns the propeller clockwise, so the propeller turns the airplane counterclockwise. Seen from the seat, that reaction is a roll to the left about the longitudinal axis, the nose-to-tail line through the center of gravity that the stability lesson introduced with the three axes. This is torque reaction: the airframe reacting to the torque the engine applies to the propeller.

On the takeoff roll that left roll has a second consequence. The rolling tendency presses down on the left main landing gear, and the harder a tire presses on the runway the more friction it develops. The left tire's extra friction drags against the airplane's forward motion on the left side, and a rearward drag on the left produces a yaw to the left. So on the ground torque reaction reaches you twice: as a roll onto the left wheel and as the left yaw that the loaded wheel's friction adds.

Designers compensate for the steady component of the roll. Older designs are rigged so the wing being forced down makes slightly more lift; more modern designs mount the engine with a slight offset. Either way the compensation is set for cruise power and airspeed, where the airplane spends most of its time, so in cruise the wings stay level without aileron pressure. At full power on takeoff the compensation is no longer matched, and torque reaction returns.

PHAK Ch 5, "Torque Reaction"

Spiraling slipstream

The propeller does not throw its air straight back. Because the blades are rotating as they push, they leave the air with a rotational twist, so the slipstream, the column of air the propeller accelerates rearward, corkscrews around the fuselage as it travels aft. Following the clockwise rotation, this spiraling slipstream wraps around and strikes the left side of the vertical stabilizer. A push on the left side of the fin yaws the nose left about the vertical axis, the same axis the fin uses to weathervane the airplane into the relative wind.

An airplane with the propeller slipstream drawn as a corkscrew wrapping around the fuselage from the propeller back to the tail, where it meets the left side of the vertical fin
The slipstream corkscrews around the fuselage and strikes the left side of the vertical fin, yawing the nose left. PHAK Figure 5-48 (FAA).

The strength of this effect depends on how tightly the slipstream is wound. At high power and low forward speed the propeller adds a large rotational twist to air that is not moving aft very fast, so the corkscrew is tight and its strike on the fin is firm. As the airplane accelerates, the same twist is stretched over a longer forward distance, the spiral loosens, and the effect weakens. That is why the spiraling slipstream is strongest in the climb and slackens in cruise.

One effect that helps The corkscrew flow also produces a rolling moment about the longitudinal axis, and that rolling moment is to the right, so it partly opposes the left roll of torque reaction. PHAK adds that these forces vary greatly with power and airspeed, so the pilot corrects what the airplane actually does rather than counting on one effect to cancel the other.

PHAK Ch 5, "Corkscrew Effect"

Gyroscopic precession

A spinning propeller is a gyroscope: a mass rotating fast enough to resist changes to its plane of rotation, and it has a gyroscope's peculiar response to a push. Gyroscopic precession is the property by which a force applied to the rim of a spinning disc takes effect not where it is applied but 90 degrees around the rim, in the direction of rotation. Push on the disc at one point and the disc responds as though you had pushed a quarter-turn later. The full behavior of gyroscopes belongs to the Unit 3 lesson on the gyroscopic flight instruments; here you need only the 90-degree rule, and only as it applies to the propeller disc.

A spinning disc with a force applied at the top and the resulting reaction shown acting at a point 90 degrees around the rim in the direction of rotation
A force applied to the rim of a spinning disc takes effect 90 degrees around the rim, in the direction of rotation. PHAK Figure 5-49 (FAA).

Apply this to the propeller. Anything that pitches or yaws the airplane applies a force to the propeller disc, and precession converts that force into a rotation about a different axis. Pitching the nose applies the force at the top or bottom of the disc, and it takes effect at the side, as a yaw. The classic case is a tailwheel airplane on the takeoff roll. As the pilot raises the tail early in the roll, the propeller disc is pitched forward, which applies a forward force at the top of the disc. On a clockwise propeller that force precesses 90 degrees around to the right side of the disc, and a forward push on the right of the disc yaws the nose left.

A tailwheel airplane on the runway raising its tail, with the forward force at the top of the propeller disc precessing to the right side and yawing the nose to the left
Raising the tail of a tailwheel airplane pitches the propeller disc forward; precession carries that force to the right of the disc and yaws the nose left. PHAK Figure 5-50 (FAA).

Precession acts only while the disc is being pitched or yawed, not while attitude is held steady, so it is a transient of the tail-raising moment on a taildragger and of any brisk pitch change. A tricycle-gear trainer keeps a level attitude during the takeoff roll and does not raise a tail, so precession is the smallest of the four tendencies in the airplane you train in. The same 90-degree rule returns in Unit 3, where it governs the gyroscopic flight instruments.

PHAK Ch 5, "Gyroscopic Action"

P-factor

The fourth tendency is P-factor, also called asymmetric loading, and it depends on the angle at which the whole airplane meets the air. When the airplane flies at a high angle of attack, as in a climb, the propeller disc is tilted back relative to the oncoming air. On the right side of the disc the blade is swinging downward as it turns, and on the left side the blade is swinging upward. Because the disc is tilted, the downswinging blade on the right meets the air at a greater angle and with a greater resultant velocity than the upswinging blade on the left.

Recall from the propeller primer above that a blade's force grows with both its angle of attack and its speed through the air. The downswinging right blade therefore produces more thrust than the upswinging left blade. The effective center of the propeller's thrust shifts to the right of the disc's center, and a thrust concentrated on the right of the nose yaws the nose left.

Two propeller discs compared: at low angle of attack the load is even across both blades, and at high angle of attack the descending right blade carries a larger load than the ascending left blade
At low angle of attack the blades load evenly; at high angle of attack the descending right blade carries more load than the ascending left, shifting thrust right and yawing the nose left. PHAK Figure 5-51 (FAA).

The condition that P-factor needs is a high aircraft angle of attack, not merely high power. At cruise the airplane flies at a low angle of attack, the disc meets the air nearly square, both sides of the disc are loaded almost equally, and P-factor nearly vanishes. It is pronounced in the climb, where power is high and the nose is up, and it is at its worst in a power-on stall, where the angle of attack is highest of all. That is why P-factor and the spiraling slipstream, not torque or precession, are the tendencies you fight hardest in the climb-out and in the power-on stalls that Stalls and Spins introduced.

PHAK Ch 5, "Asymmetric Loading (P-Factor)"

The four together in the cockpit

The four tendencies do not arrive equally at once; which one dominates depends on what the airplane is doing.

The correction is the same in every case: right rudder, fed in by feel until the nose stops drifting and stays where you point it. You do not compute which tendency is acting or how much; you watch the nose, and you hold enough right rudder to keep the airplane in coordinated flight. As power comes back and speed builds, all four tendencies weaken together, and the pressure you hold eases off.

A different left-yaw effect Rolling into a turn also yaws the nose, but that effect, called adverse yaw, comes from the drag of the deflected ailerons rather than the propeller, so it is not one of the four left-turning tendencies.
Where the tendencies bite The tendencies are strongest at high power, high angle of attack, and low airspeed, which is the exact condition of a power-on stall. Letting the nose yaw left there, with the wing near its critical angle, is how a stall becomes a spin. Keeping the airplane coordinated with right rudder in the climb and in power-on stalls is what keeps a stall from dropping a wing.

This closes Unit 2. You now have the forces on the airplane, the wing that makes lift, the drag that resists it, the stall and spin, the airplane's stability, the load factor in turns, and the propeller's pull on the nose. Next comes the machine that spins that propeller: Unit 3 opens with The Engine and Propeller.

PHAK Ch 5, "Torque and P-Factor"

Why this matters in the airplane Right rudder on takeoff and in the climb is the first habit your instructor will build, and these four causes are why. On the takeoff roll, lead with right rudder as the power comes in, because torque-loaded tire friction and the slipstream are already yawing you left. In the climb and in every power-on stall, hold the right rudder that keeps the ball centered, because P-factor and the slipstream are strongest there and an uncoordinated stall drops a wing. You judge the amount by the nose and the ball, holding whatever right rudder keeps them steady.

Check your understanding

Answer from memory, without scrolling back up. Recalling it yourself is what makes it stick.

The four left-turning tendencies are?

Torque reaction rolls the airplane which way, and about which axis?

On the takeoff roll, torque reaction produces a left yaw because?

The spiraling slipstream yaws the nose left because it?

The spiraling slipstream effect is strongest when?

Gyroscopic precession makes an applied force take effect?

Raising the tail of a tailwheel airplane yaws it left because?

P-factor arises at high angle of attack because?

P-factor is most pronounced in which condition?

The pilot's correction for all four tendencies is?

Go deeper (primary source): read the "Torque and P-Factor" section of PHAK Chapter 5, covering torque reaction, the corkscrew effect, gyroscopic action, and asymmetric loading. The propeller that produces all four is the subject of the next lesson, The Engine and Propeller, which opens Unit 3.

Stuck or curious? On your next flight, ask your instructor to let you feel the right rudder needed at three moments: as the power comes up on the takeoff roll, during a full-power climb, and in a power-on stall entry. Notice how the pressure grows as the airplane slows and the nose comes up, and how it eases as speed returns.