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The work done by a variable force acting over a finite linear displacement ... The equation for the magnitude of a torque, arising from a perpendicular force:
The work done is given by the dot product of the two vectors, where the result is a scalar. When the force F is constant and the angle θ between the force and the displacement s is also constant, then the work done is given by: = If the force is variable, then work is given by the line integral:
The work done W by an external agent which exerts a force F (at r) and torque τ on an object along a curved path C is: W = Δ T = ∫ C ( F ⋅ d r + τ ⋅ n d θ ) {\displaystyle W=\Delta T=\int _{C}\left(\mathbf {F} \cdot \mathrm {d} \mathbf {r} +{\boldsymbol {\tau }}\cdot \mathbf {n} \,{\mathrm {d} \theta }\right)}
The work done by the force ... The mechanical advantage of the gear train is the ratio of the output torque T B to the input torque T A, and the above equation yields ...
The equation for torque is very important in angular mechanics. Torque is rotational force and is determined by a cross product. This makes it a pseudovector. = where is torque, r is radius, and is a cross product. Another variation of this equation is:
When friction is included, the mechanical advantage is no longer equal to the distance ratio but also depends on the screw's efficiency. From conservation of energy, the work W in done on the screw by the input force turning it is equal to the sum of the work done moving the load W out, and the work dissipated as heat by friction W fric in the ...
The work done by a torque acting on an object equals the magnitude of the torque times the angle through which the torque is applied: =. The power of a torque is equal to the work done by the torque per unit time, hence: P = τ ω . {\displaystyle P=\tau \omega .}
Torque is the rotation equivalent of force in the same way that angle is the rotational equivalent for position, angular velocity for velocity, and angular momentum for momentum. As a consequence of Newton's first law of motion, there exists rotational inertia that ensures that all bodies maintain their angular momentum unless acted upon by an ...