For kinetic energy
m d v x d t = F x → d d t ( m v x 2 2 ) = F x v x → d ( m v x 2 2 ) = F x d x → m\frac{dv_x}{dt}=F_x\to\frac{d}{dt}(\frac{mv_x^2}{2})=F_xv_x \to d(\frac{mv_x^2}{2})=F_xdx\to m d t d v x = F x → d t d ( 2 m v x 2 ) = F x v x → d ( 2 m v x 2 ) = F x d x →
m v x f 2 2 − m v x 0 2 2 = ∫ F x d x \frac{mv_{xf}^2}{2}-\frac{mv_{x0}^2}{2}=\int F_xdx 2 m v x f 2 − 2 m v x 0 2 = ∫ F x d x . In general m v f 2 2 − m v 0 2 2 = ∫ F ⃗ d r ⃗ \frac{mv_{f}^2}{2}-\frac{mv_{0}^2}{2}=\int \vec Fd\vec r 2 m v f 2 − 2 m v 0 2 = ∫ F d r
For potential energy
F ⃗ d r ⃗ = − ∂ E p ∂ x d x − ∂ E p ∂ y d y − ∂ E p ∂ z d z → F ⃗ d r ⃗ = − d E p → \vec Fd\vec r=-\frac{\partial E_p}{\partial x}dx-\frac{\partial E_p}{\partial y}dy-\frac{\partial E_p}{\partial z}dz \to \vec Fd\vec r=-dE_p \to F d r = − ∂ x ∂ E p d x − ∂ y ∂ E p d y − ∂ z ∂ E p d z → F d r = − d E p →
− ( E p 2 − E p 1 ) = ∫ F ⃗ d r ⃗ -(E_{p2}-E_{p1})=\int \vec Fd\vec r − ( E p 2 − E p 1 ) = ∫ F d r
If the body has both potential and kinetic energy then
W = ∫ F ⃗ d r ⃗ = m v f 2 2 − m v 0 2 2 − ( − ( E p 2 − E p 1 ) ) = W=\int \vec Fd\vec r=\frac{mv_{f}^2}{2}-\frac{mv_{0}^2}{2}-(-(E_{p2}-E_{p1}))= W = ∫ F d r = 2 m v f 2 − 2 m v 0 2 − ( − ( E p 2 − E p 1 )) =
= ( m v f 2 2 + E p 2 ) − ( m v 0 2 2 + E p 1 ) =(\frac{mv_{f}^2}{2}+E_{p2})-(\frac{mv_{0}^2}{2}+E_{p1}) = ( 2 m v f 2 + E p 2 ) − ( 2 m v 0 2 + E p 1 ) .
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