Work
Suppose that a particle subject to a force
undergoes an infinitesimal displacement
. The
net work that the force does on the particle (i.e., the net energy transferred to the body by the force) is
![$\displaystyle dW = {\bf f}\cdot d{\bf r}.$](img184.png) |
(1.28) |
(See Section A.6.)
In other words, the work is the product of the displacement and the component of the force parallel to the
displacement.
It follows from Equation (1.22) that
![$\displaystyle dW = m\,\frac{d{\bf v}}{dt}\,\cdot d{\bf r}.$](img185.png) |
(1.29) |
However,
, so we obtain
![$\displaystyle dW = m\,\frac{d{\bf v}}{dt}\,\cdot{\bf v}\,dt = m\,{\bf v}\cdot d{\bf v}.$](img187.png) |
(1.30) |
Furthermore,
![$\displaystyle {\bf v}\cdot d{\bf v} = v_x\,dv_x + v_y\,dv_y + v_z\,dv_z = \frac...
...) + \frac{1}{2}\,d(v_y^{\,2})+ \frac{1}{2}\,d(v_z^{\,2}) = \frac{1}{2}\,d(v^2),$](img188.png) |
(1.31) |
where
is the particle's speed. It follows from the previous two equations that
![$\displaystyle dW = dK,$](img190.png) |
(1.32) |
where
![$\displaystyle K = \frac{1}{2}\,m\,v^{\,2}.$](img191.png) |
(1.33) |
Here,
is known as kinetic energy, and is the energy that the particle possesses by virtue of its motion.
Equation (1.32) can be integrated to give the work-energy theorem,
![$\displaystyle W= {\mit\Delta} K.$](img192.png) |
(1.34) |
According to this theorem, the net work done by the force acting on the particle in a given time interval is
equal to the change in the particle's kinetic energy during the same time interval.
Suppose that the force is a function of the particle's displacement,
.
If the particle moves from point
to
point
along any path then Equations (1.28) and (1.34) imply that
![$\displaystyle W = \int_{{\bf r}_A}^{{\bf r}_B}{\bf f}\cdot d{\bf r} = K_B-K_A,$](img194.png) |
(1.35) |
where
denotes the displacement of
point
, et cetera,
is the kinetic energy at point
, et cetera, and
is an element of the path. (See Section A.14.)