Figure P3.40 illustrates a pendulum with a base that moves horizontally. This is a simple model of an overhead crane carrying a suspended load with cables. The load mass is m, the cable length is L, and the base acceleration is a(t). Assuming that the cable acts like a rigid rod, derive the equation of motion in terms of ? with a(t) as the input.
Figure P3.40 illustrates a pendulum with a base that moves horizontally. This
is a simple model of an overhead crane carrying a suspended load with cables.
The load mass is m, the cable length is L, and the base acceleration is a(t).
Assuming that the cable acts like a rigid rod, derive the equation of motion in
terms of ? with a(t) as the input.


To derive the equation of motion for the pendulum with a base that moves horizontally, we can use the Lagrangian approach.
Let be the angle between the cable and the vertical, and let x be the horizontal displacement of the base. The kinetic and potential energies of the system can be expressed as:
Kinetic Energy: T = ((1/2)m (L2)) + ((1/2)m2)
Potential Energy: V = -mgL cos()
where and are the time derivatives of and x, respectively.
The Lagrangian of the system is given by:
L = T - V = ((1/2)m(L2)) + ((1/2)m2)+ mgL cos()
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