Lagrange's equations to Newton's equations

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The discussion focuses on demonstrating how Lagrange's equations reduce to Newton's equations of motion when using Cartesian coordinates as generalized coordinates. The Lagrangian is defined as L = T - V, with kinetic energy T and potential energy V expressed in terms of the system's coordinates. A key point made is that when substituting into Lagrange's equations, the resulting equation for motion shows that mass times acceleration equals the negative derivative of the potential, which aligns with Newton's second law. The conversation also distinguishes between conservative forces, derived from potential energy, and non-conservative forces represented by external inputs. Ultimately, the participants clarify that the Lagrange equation can indeed lead to Newton's second law under the right conditions.
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I want to show the Lagrange's equations reduces to Newton's equation of motion if we take the Cartesian coordinates as the generalised coordinates.

So let T be the K.E. of the system and V be the P.E. of the system. So the Lagrangian is L=T-V.

So T = \frac{1}{2}m(\dot{x}^2 + \dot{y}^2 + \dot{z}^2)

& V = V(x,y,z)
Help me proceed with the proof :frown:.
 
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Actually,

<br /> T = \frac{1}{2}m \left( \dot{x}^2 + \dot{y}^2 + \dot{z}^2 \right).<br />

What do you get when you substitute T and V[/tex] into Lagrange&#039;s equations?<br /> <br /> Regards,<br /> George
 
Sorry for the typo and thank you replying. I made the substitution in Lagrange's equation.
\frac{d}{dt} \left(\frac{\partial L}{\partial \dot{q_i}}\right) - \frac{\partial L}{\partial \dot{q_i}}= Q_i&#039;

Setting q1=x,q2=y,q3=z

I get the Lagrange's equation for variable x as:
m\ddot{x} + \frac{\partial V}{\partial x} = Q_1&#039;

How does this equation show Newton's second law of motion?
 
What is

<br /> -\frac{\partial V}{\partial x}?<br />

Regards,
George
 
Umm...is it part of the net force?
 
Reshma said:
Umm...is it part of the net force?

Yes. What is the force that results from a potential V=V\left(x,y,z\right), and what type of force is it?

Regards,
George
 
YOUR LAGRANGE EQUATION IS NOT RIGHT. THERE SOULD BE ZERO ON THE WRITE HAND SIDE NOT Q. AGAIN IF YOU PUT Q=0 IN YOUR SECOND EQUATION YOU GET;
MASS X ACCELERATION = - THE DIREVATIVE OF THE POTENTIAL WITH RESPECT TO x.
= FORCE.
ISN'T THIS THE SECOND LAW OF NEWTON?
 
samalkhaiat said:
YOUR LAGRANGE EQUATION IS NOT RIGHT. THERE SOULD BE ZERO ON THE WRITE HAND SIDE NOT Q. AGAIN IF YOU PUT Q=0 IN YOUR SECOND EQUATION YOU GET;
MASS X ACCELERATION = - THE DIREVATIVE OF THE POTENTIAL WITH RESPECT TO x.
= FORCE.
ISN'T THIS THE SECOND LAW OF NEWTON?

The terms involving the potential and the terms involving the Q' s represent different types of forces. This is what I was trying to point the way towards in my last post.

Regards,
George
 
Thank you very much for all your replies.
George Jones said:
Yes. What is the force that results from a potential V=V\left(x,y,z\right), and what type of force is it?

Regards,
George
There is part of the force derivable from PE and the other part independent of the PE. So one has to be the conservative part and the other the non-conservative part. So Q's represent the non-conservative parts and V(x,y,z) represent the conservative part, right? Can you elaborate more on these forces?
 
  • #10
samalkhaiat said:
YOUR LAGRANGE EQUATION IS NOT RIGHT. THERE SOULD BE ZERO ON THE WRITE HAND SIDE NOT Q. AGAIN IF YOU PUT Q=0 IN YOUR SECOND EQUATION YOU GET;
MASS X ACCELERATION = - THE DIREVATIVE OF THE POTENTIAL WITH RESPECT TO x.
= FORCE.
ISN'T THIS THE SECOND LAW OF NEWTON?
Be easy on the Caps :wink:!
 
  • #11
so you wrote down Lagrange equation with a source on the right hand side of it. Then you ask about deriving Newton second law from it. But you actually did derive it.
The forces as you said conservative (derivable from potential) and non-conservative (which are not) like friction forces etc.
 
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