Yaw (rotation)
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A yaw rotation is a movement around the yaw axis of a rigid body that changes the direction it is pointing, to the left or right of its direction of motion. The yaw rate or yaw velocity of a car, aircraft, projectile or other rigid body is the angular velocity of this rotation, or rate of change of the heading angle when the aircraft is horizontal. It is commonly measured in degrees per second or radians per second. Another important concept is the yaw moment, or yawing moment, which is the component of a torque about the yaw axis.


Measurement

Yaw velocity can be measured by measuring the ground velocity at two geometrically separated points on the body, or by a
gyroscope A gyroscope (from Ancient Greek γῦρος ''gŷros'', "round" and σκοπέω ''skopéō'', "to look") is a device used for measuring or maintaining Orientation (geometry), orientation and angular velocity. It is a spinning wheel or disc in ...
, or it can be synthesized from accelerometers and the like. It is the primary measure of how drivers sense a car's turning visually. It is important in electronic stabilized vehicles. The yaw rate is directly related to the lateral acceleration of the vehicle turning at constant speed around a constant radius, by the relationship :tangential speed*yaw velocity = lateral acceleration = tangential speed^2/radius of turn, in appropriate units The sign convention can be established by rigorous attention to coordinate systems. In a more general manoeuvre where the radius is varying, and/or the speed is varying, the above relationship no longer holds.


Yaw rate control

The yaw rate can be measured with accelerometers in the vertical axis. Any device intended to measure the yaw rate is called a yaw rate sensor.


Road vehicles

Studying the stability of a road vehicle requires a reasonable approximation to the equations of motion. The diagram illustrates a four-wheel vehicle, in which the front axle is located ''a'' metres ahead of the centre of gravity and the rear axle is ''b'' metres towards the rear from the center of gravity. The body of the car is pointing in a direction \theta (theta) while it is travelling in a direction \psi (psi). In general, these are not the same. The tyre treads at the region of contact point in the direction of travel, but the hubs are aligned with the vehicle body, with the
steering Steering is the control of the direction of motion or the components that enable its control. Steering is achieved through various arrangements, among them ailerons for airplanes, rudders for boats, cylic tilting of rotors for helicopters, ...
held central. The tyres distort as they rotate to accommodate this mis-alignment, and generate side forces as a consequence. From directional stability study, denoting the angular velocity \omega, the equations of motion are: :\frac=2k\frac\beta-2k\frac\omega :\frac=-\frac\beta+(1-2k)\frac\omega with M the mass of the vehicle, V the vehicle speed and \beta = \theta - \psi the vehicle's overall angle. The coefficient of \frac will be called the ' damping' by analogy with a mass-spring-damper which has a similar equation of motion. By the same analogy, the coefficient of \beta will be called the 'stiffness', as its function is to return the system to zero deflection, in the same manner as a spring. The form of the solution depends only on the signs of the damping and stiffness terms. The four possible solution types are presented in the figure. The only satisfactory solution requires both stiffness and damping to be positive. If the centre of gravity is ahead of the centre of the wheelbase (b>a), this will always be positive, and the vehicle will be stable at all speeds. However, if it lies further aft, the term has the potential of becoming negative above a speed given by: ::V^2=\frac Above this speed, the vehicle will be directionally (yaw)
unstable In dynamical systems instability means that some of the outputs or internal state (controls), states increase with time, without bounds. Not all systems that are not Stability theory, stable are unstable; systems can also be marginal stability ...
. Corrections for relative effect of front and rear tyres and steering forces are available in the main article.


Relationship with other rotation systems

These rotations are intrinsic rotations and the calculus behind them is similar to the Frenet-Serret formulas. Performing a rotation in an intrinsic reference frame is equivalent to right-multiply its characteristic matrix (the matrix that has the vector of the reference frame as columns) by the matrix of the rotation.


History

The first aircraft to demonstrate active control about all three axes was the Wright brothers' 1902 glider.{{cite web , url=https://www.grc.nasa.gov/WWW/K-12/airplane/rotations.html , title=Aircraft rotations , date=2015-05-05 , publisher=
Glenn Research Center NASA John H. Glenn Research Center at Lewis Field is a NASA center within the cities of Brook Park, Ohio, Brook Park and Cleveland between Cleveland Hopkins International Airport and the Rocky River Reservation of Cleveland Metroparks, with a s ...
, access-date=2018-10-13


See also

* Adverse yaw * Aircraft principal axes * Coriolis acceleration * Directional stability *
Flight dynamics Flight dynamics in aviation and spacecraft, is the study of the performance, stability, and control of vehicles flight, flying through the air or in outer space. It is concerned with how forces acting on the vehicle determine its velocity and at ...
* Six degrees of freedom * Vehicle dynamics * Yaw rate sensor


References

Dynamics (mechanics) Attitude control