The displacement can be divided into a large number of small equal displacements ∆x. During a small displacement ∆x, the force F can be assumed to be constant. Then the work done is
W =~ F.∆x = Area of rectangle abcd.
In the limit when ∆x→0, the number of rectangles tends to be infinite, but the above summation approaches to a definite integral whose value is equal to the area under the curve. Thus the total work done is
Hence, for a varying force the work done is equal to the definite integral of the force over the given displacement.
Tags
Work Energy & Power


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