When do I need to use virtual work in writing the equations of motion?

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SUMMARY

The discussion focuses on the application of the principle of virtual work in Lagrangian dynamics, specifically in the context of the Euler-Lagrange equations. The equation of motion is established as \(\frac{d}{dt}\frac{\partial L}{\partial\dot{q}_{i}} = \frac{\partial L}{\partial {q}_{i}}\). The principle of virtual work is introduced to account for non-conservative forces, leading to the modified equation \(\frac{d}{dt}\frac{\partial L}{\partial\dot{q}_{i}} - \frac{\partial L}{\partial {q}_{i}} = F_{q}\), where \(F_{q}\) represents the generalized non-conservative forces. The discussion clarifies that \(F_{q}\) is essential when non-conservative forces are present, allowing for accurate modeling of motion.

PREREQUISITES
  • Understanding of Lagrangian dynamics and the Euler-Lagrange equations
  • Familiarity with generalized coordinates and forces in mechanics
  • Knowledge of non-conservative forces and their impact on motion
  • Basic proficiency in calculus, particularly differentiation with respect to time
NEXT STEPS
  • Study the derivation and applications of the Euler-Lagrange equations in detail
  • Explore the principle of virtual work and its implications in mechanics
  • Investigate examples of non-conservative forces and their representation in Lagrangian mechanics
  • Review advanced topics in Lagrangian dynamics, including modified equations for complex systems
USEFUL FOR

Students preparing for comprehensive exams in mechanical engineering, researchers in dynamics, and anyone seeking to deepen their understanding of Lagrangian mechanics and the role of virtual work in motion equations.

jhosamelly
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I'm studying for our comprehensive exam . I just need to clarify something. So the equation of motion for lagrangian dynamics is \frac{d}{dt}\frac{\partial L}{\partial\dot{q}_{i}} = \frac{\partial L}{\partial {q}_{i}}

However, in my notes there are example which uses the principle of virtual work wherein \frac{d}{dt}\frac{\partial L}{\partial\dot{q}_{i}} - \frac{\partial L}{\partial {q}_{i}} = F_{q}

Then we look for F_{q} using virtual work.

However isn't \frac{d}{dt}\frac{\partial L}{\partial\dot{q}_{i}} - \frac{\partial L}{\partial {q}_{i}} = 0 ?
 
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I think I can help you, but I don't want to answer without knowing what F sub q stands for just in case I make things worse. Can you specify what it represents please?
 
q is the generalized coordinate.

For example if I have r (radial distance) as generalized coordinate I'll have


\frac{d}{dt}\frac{\partial L}{\partial\dot{r}} - \frac{\partial L}{\partial {r}} = F_{r}
 

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