Problem in getting correct coefficients of frictional forces

AI Thread Summary
The discussion centers on challenges faced when applying the Lagrangian method to systems with friction, particularly regarding the correct coefficients of frictional forces. Users note that while Lagrangian mechanics works well for conservative systems, it struggles with dissipative forces like friction. There is confusion about the distinction between generalized forces and regular forces, with emphasis on the need to correctly account for these in equations. One participant references Goldstein's text for guidance on handling such systems, suggesting that many students may not fully grasp advanced applications of Lagrangian mechanics. The conversation highlights the importance of understanding the nuances of applying Lagrangian methods to systems involving friction.
Amitayas Banerjee
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I am getting correct equations on using the Lagrangian method in Systems with no non conservative forces, but when I use it in Systems with friction, sometimes I get correct equations, and sometimes I do not. Most of the equations have some problem with the coefficients of the frictional forces.
For example, let us take a look at this system...
ss3iS.jpg


Here f1,f2 are the frictional forces(and not the coefficients of friction)

Now, let the block with mass $m_2$ move through a distance $x$ to ward the right.
Vqyxs.jpg


now, when we apply Newton's second law, we see that this is wrong and the coefficient of f1should have been 2
Why is the problem?...on the right hand side I have written the generalized force and the the two Lagrangian terms on the left hand side. Please help me out.
 

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Standard Lagrangian mechanics does not handle dissipative systems.
 
Orodruin said:
Standard Lagrangian mechanics does not handle dissipative systems.
I have not used that...I have used the version with generalized forces(RHS has got -f1-f2)
 
Amitayas Banerjee said:
I have not used that...I have used the version with generalized forces(RHS has got -f1-f2)
The RHS that you wrote is not the generalized forces, it is the regular forces. The generalized forces are
$$F_i \cdot \frac{\partial v_i}{\partial \dot{q_j}}$$
That is where the factor of 2 comes in
 
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Dale said:
The RHS that you wrote is not the generalized forces, it is the regular forces. The generalized forces are
$$F_i \cdot \frac{\partial v_i}{\partial \dot{q_j}}$$
That is where the factor of 2 comes in
Sirl, is that vi=xdot i?
 
Orodruin said:
Standard Lagrangian mechanics does not handle dissipative systems.

I'm not sure what "standard" means in this context, but I use Lagrange frequently for systems involving losses. See Goldstein, pp. 38 - 40.
 
Amitayas Banerjee said:
Sirl, is that vi=xdot i?
@Dr.D Sir, can you clarify this?
 
Amitayas Banerjee said:
Sirl, is that vi=xdot i?
Yes
 
Dr.D said:
I'm not sure what "standard" means in this context, but I use Lagrange frequently for systems involving losses. See Goldstein, pp. 38 - 40.
What edition are you using? Pages 38 to 40 in my Goldstein is just general variational calculus.

Anyway, I read the OP and replied a bit fast it seems. By "standard" I was meaning only letting the variation of an action be equal to zero, which is what most students learn first and many do not go beyond. For some reason I thought the OP was trying to do something like trying to introduce friction forces in the Lagrangian.
 
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Orodruin said:
What edition are you using?
There is no edition number in my copy, only a 1959 copyright date and the notation 6th printing. For this reason, I presume it is a 1st edition. I used it as a textbook in the school year 1963-64. I've been using this to good effect ever since.
 
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