Also, the magnitude of the torque is greater when the lever arm is longer. But if the object can rotate about point B, it will rotate clockwise, which means the torque for the force shown is clockwise relative to B. If the object can rotate about point A, it will rotate counterclockwise, which means that the torque for the force is shown as counterclockwise relative to A. Torque is either clockwise or counterclockwise relative to the chosen pivot point, as illustrated for points B and A, respectively, in Figure 9.7. Note that for rotation in a plane, torque has two possible directions. The object may not actually pivot about the chosen “pivot point.” Any point in any object can be chosen to calculate the torque about that point. For the same applied force, a different choice for the location of the pivot will give you a different value for the torque, since both r r and θ θ depend on the location of the pivot. The torque is always calculated with reference to some chosen pivot point. If you reduce the force to 20 N, the torque is reduced to 16 N m(0.800 m × 40 N × sin 90º) relative to the hinges.For example, if you push perpendicular to the door with a force of 40 N at a distance of 0.800 m from the hinges, you exert a torque of 32 N The SI unit of torque is newtons times meters, usually written as N Τ = rF sin θ τ = rF sin θ for torque, but both are equally valid. In such cases, it may be more convenient to use It is sometimes easier to find or visualize Note that the line segment that defines the distanceį F, as its name implies. The perpendicular lever arm r ⊥ r ⊥ is the shortest distance from the pivot point to the line along whichį F acts it is shown as a dashed line in Figure 9.6 and Figure 9.7. The torque from the applied force will cause a clockwise rotation around point B, and so it is a clockwise torque relative to B. (b) In this case, point B is the pivot point. This means that torque is counterclockwise relative to pivot A.

If the object can rotate around point A, it will rotate counterclockwise. (a) The three factors r r, F F, and θ θ for pivot point A on a body are shown here- r r is the distance from the chosen pivot point to the point where the force F F is applied, and θ θ is the angle between F F and the vector directed from the point of application to the pivot point. In equation form, the magnitude of torque is defined to beįigure 9.7 A force applied to an object can produce a torque, which depends on the location of the pivot point. It is a measure of the effectiveness of a force in changing or accelerating a rotation (changing the angular velocity over a period of time). Torque is the rotational equivalent of a force. The magnitude, direction, and point of application of the force are incorporated into the definition of the physical quantity called torque. (f) Torque is zero here since the force just pulls on the hinges, producing no rotation. (e) A smaller counterclockwise torque is produced by the same magnitude force acting at the same point but in a different direction. (d) The same force as in (a), but acting in the opposite direction, produces a clockwise torque. (c) The same force as in (a) produces a smaller counterclockwise torque when applied at a smaller distance from the hinges. (b) A smaller counterclockwise torque is produced by a smaller force F′ F′ acting at the same distance from the hinges (the pivot point). Note that r ⊥ r ⊥ is the perpendicular distance of the pivot from the line of action of the force. (a) Counterclockwise torque is produced by this force, which means that the door will rotate in a counterclockwise due to F F. The most effective direction is perpendicular to the door-we push in this direction almost instinctively.įigure 9.6 Torque is the turning or twisting effectiveness of a force, illustrated here for door rotation on its hinges (as viewed from overhead). Finally, the direction in which you push is also important. Most people have been embarrassed by making this mistake and bumping up against a door when it did not open as quickly as expected. If you apply your force too close to the hinges, the door will open slowly, if at all.

Also, the point at which you push is crucial. First of all, the larger the force, the more effective it is in opening the door-obviously, the harder you push, the more rapidly the door opens. Several familiar factors determine how effective you are in opening the door. To understand what factors affect rotation, let us think about what happens when you open an ordinary door by rotating it on its hinges. A rotating body or system can be in equilibrium if its rate of rotation is constant and remains unchanged by the forces acting on it. The second condition necessary to achieve equilibrium involves avoiding accelerated rotation (maintaining a constant angular velocity).

3d problems of static equilibrium