Work
Work done by a constant force
Only the component of a force in the direction of the displacement does work. If the force is constant, then we can simplify the general work equation to the following.
U1-2 = F⋅Δr1-2 or U1-2 = Fcosθ d1-2
Work done by a non-constant force
The general work equation may be applied in the individual coordinate directions.
U1-2 = ∫Fxdx + ∫Fydy
Work in the n-t coordinate system
Since motion only occurs in the t-direction, only the t-component of the force does work.
U1-2 = ∫Ftds