When the pendulum just barely completes a
circular motion around its pivot, the tension in the string at the topmost
point of the circular path is zero. At the top of the circle, the only force
acting on the pendulum bob is its weight .
The centripetal force required to complete
the circular motion at the top is provided by the weight of the bob. The
centripetal force , where is the speed of the bob at
the top of the circle and is the length of the pendulum.
At the top of the circle, , so
, which gives
.
Use the conservation of mechanical energy
to find the energy at the bottom:
The total mechanical energy of the pendulum
is conserved. Let's consider the potential energy at the top of the circle and
the kinetic energy at the bottom of the circle.
The potential energy at the top of the
circle with respect to the bottom of the circle is