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Work done by constant force at an angle 0 to the straight-line displacement (6-2)

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Question

Angle between the directions of \boldsymbol{\vec{F}} and \boldsymbol{\vec{d}}

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Review

How can we calculate the work done by a constant force that is not in the direction of the object’s motion? As an example, in Figure 6-6a a groundskeeper is using a rope to pull a screen across a baseball diamond to smooth out the dirt. The net tension force \vec{F} that the rope exerts on the screen is at an angle with respect to the direction in which the screen moves. In such a case, only the component of the force along the direction of motion contributes to the work done (Figure 6-6b).

If \theta is the angle between the force \vec{F} and the displacement \vec{d}, this component of the force is F \cos \theta. Hence the amount of work done by the force is: