3D pendulum-spring-damper (Lagrange)

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SUMMARY

The discussion focuses on deriving the equations of motion for a 3D pendulum-spring-damper system using Lagrange's formulation. The generalized coordinates are defined as \(\vec{q}=[x,y,z]^T\). Key equations presented include the position vector \(\vec{r}\), velocity vector \(\vec{v}\), kinetic energy \(T\), dissipation function \(D\), and potential energy \(V\). The user seeks verification of the correctness of these expressions, particularly the potential energy equation.

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Homework Statement



I need to find the equations of motions via Lagrange's formulation when the generalized coordinates are:
[tex]\vec{q}=[x,y,z]^T[/tex]2. The attempt at a solution

I need to verify whether what I obtained so far is true or not.

The position vector if the bob (from the support) is:[tex]\vec{r}=x\hat{e}_{1}+y\hat{e}_2+(L-z)\hat{e}_{3}[/tex]

And the velocity vector is: [tex]\vec{v}=\dot{x}\hat{e}_{1}+\dot{y}\hat{e}_{2}-\dot{z}\hat{e}_{3}[/tex]

The Kinetic energy is: [tex]T=\frac{1}{2}mv^{2}=\frac{1}{2}m(\dot{x}^{2}+\dot{y}^{2}+\dot{z}^{2})[/tex]

The dissipation function is: [tex]D=\frac{1}{2}C(\dot{x}^{2}+\dot{y}^{2}+\dot{z}^{2})[/tex]

The potential energy (gravitational energy is taken with respect to the support) is: [tex]V=-mg(L-z)+\frac{1}{2}k\left ( \sqrt{x^{2}+y^{2}+(L-z)^{2}}-l_{0} \right )^{2}[/tex]

The generalized forces (given in the original question): [tex]Q_{x}=F_{x}[/tex] , [tex]Q_{y}=F_{y}[/tex] , [tex]Q_{z}=0[/tex]

Each of these expression will be substituted into Lagrange's equation of motion:

[tex]\frac{d}{dt}\left ( \frac{\partial T}{\partial \dot{q_j}} \right )-\frac{\partial T}{\partial q_j}+\frac{\partial V}{\partial q_j}+\frac{\partial D}{\partial \dot{q_j}}=Q_j[/tex]

Are those expressions, especially that one of the potential energy, correct?

Thanks!
 
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