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In physics and mechanics, torque is the rotational analogue of linear force. [1] It is also referred to as the moment of force (also abbreviated to moment ). The symbol for torque is typically τ {\displaystyle {\boldsymbol {\tau }}} , the lowercase Greek letter tau .
Torsion of a square section bar Example of torsion mechanics. In the field of solid mechanics, torsion is the twisting of an object due to an applied torque [1] [2].Torsion could be defined as strain [3] [4] or angular deformation [5], and is measured by the angle a chosen section is rotated from its equilibrium position [6].
Torque when one end of a 1 m long moment arm is acted upon by a force of 1 N. 10^2: 108 N⋅m to 149 N⋅m: 80 lb⋅ft to 110 lb⋅ft: Torque to which most lug nuts are tightened. [1] 10^2: 881 N⋅m: 650 lb⋅ft: Torque at the crankshaft of a Dodge Charger SRT HellCat. [2] 10^4 13,000 N⋅m Example 2 MW wind turbine, generator side. [3] 10^6 ...
Moments are usually defined with respect to a fixed reference point and refer to physical quantities located some distance from the reference point. For example, the moment of force, often called torque, is the product of a force on an object and the distance from the reference point to the object. In principle, any physical quantity can be ...
A few examples are: The forces exerted by one's hand on a screw-driver; The forces exerted by the tip of a screwdriver on the head of a screw; Drag forces acting on a spinning propeller; Forces on an electric dipole in a uniform electric field; The reaction control system on a spacecraft; Force exerted by hands on steering wheel
Torque-free precessions are non-trivial solution for the situation where the torque on the right hand side is zero. When I is not constant in the external reference frame (i.e. the body is moving and its inertia tensor is not constantly diagonal) then I cannot be pulled through the derivative operator acting on L.
Physical examples of pseudovectors include torque, [4] angular velocity, angular momentum, [4] magnetic field, [4] vorticity and magnetic dipole moment. Each wheel of the car on the left driving away from an observer has an angular momentum pseudovector pointing left. The same is true for the mirror image of the car.
In 1820, the French engineer A. Duleau derived analytically that the torsion constant of a beam is identical to the second moment of area normal to the section J zz, which has an exact analytic equation, by assuming that a plane section before twisting remains planar after twisting, and a diameter remains a straight line.