The concept of torque in physics originated with the work of Archimedes on levers. Informally, torque can be though of as "rotational force". The weight that rests on a lever, multiplied by its distance from the lever's fulcrum, is the torque. For example, three pounds resting two feet from the fulcrum exerts the same torque as one pound resting six feet from the fulcrum. This assumes the force is in a direction at right angles to a straight lever. More generally, one may define torque as the cross product τ = r×F, where r is the vector from the axis of rotation to the point on which the force is acting, and F is the vector of force. Torque is important in the design of machines such as engines.
Torque has dimensions of distance × force; the same as energy. However, the units of torque are usually stated as "newton metres" or "foot pounds" rather than joules. Of course this is not simply a coincidence  a torque of 1 Nm applied through a full revolution will require an energy of exactly 2π J — mathematically, E = τ θ, where E is the energy and θ is the angle moved, in radians.
A very useful special case, often given as the definition of torque in fields other than physics, is as follows:
The construction of the "moment arm" is shown in the figure below, along with the vectors r and F mentioned above. The problem with this definition is that it does not give the direction of the torque, and hence it is difficult to use in three dimensional cases. Note that if the force is perpendicular to the displacement vector r, the moment arm will be equal to the distance to the centre, and torque will be a maximum. This gives rise to the approximation
For example, if a person places a force of 9.8 N (1 kg) on a spanner which is 0.5 m long, the torque will be approximately 4.9 Nm, assuming that the person pulls the spanner in the direction best suited to turning bolts.
Torque is the timederivative of angular momentum, just as force is the time derivative of linear momentum. For multiple torques acting simultaneously:
<math>\sum\boldsymbol{\tau} ={d\mathbf{L} \over dt}</math>
where L is angular momentum. See also proof of angular momentum.
Torque on a rigid body can be written in terms of rotational inertia I: L = Iω so if I is constant,
<math>\boldsymbol{\tau}=I{d\boldsymbol{\omega} \over dt}=I\boldsymbol{\alpha}</math>
where α is angular acceleration, a quantity usually measured in rad/s^{2}.
The measurement of torque is important in automotive engineering, being concerned with the transmission of power from the drive train to the wheels of a vehicle. It is also used where the tightness of screws and bolts is crucial (see torque wrench[?]). Torque is also the easiest way to explain mechanical advantage in just about every simple machine except the pulley.
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