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.

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
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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
a
P
0
00
g
L
УА
m
X
Transcribed Image Text:Figure P3.40 a P 0 00 g L УА m X
Expert Solution
Step 1

To derive the equation of motion for the pendulum with a base that moves horizontally, we can use the Lagrangian approach.

Let θ 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 ×(L×θ.2)) + ((1/2)×m×x.2)

Potential Energy: V = -mgL cos(θ)

where θ.and x. are the time derivatives of θ and x, respectively.

The Lagrangian of the system is given by:

L = T - V = ((1/2)×m×(Lθ.2)) + ((1/2)×m×x.2)+ mgL cos(θ)

 

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