I Potentials of conservative forces

AI Thread Summary
The discussion centers on the definition of conservative forces and potentials, specifically questioning whether potentials of the form V(r, \dot{r}) can be considered conservative. It is noted that a conservative force is defined by having a closed loop integral equal to zero, which suggests that V(r, \dot{r}) would not qualify as conservative. The conversation also touches on the implications of Goldstein's work and the relationship between time independence in Lagrangian mechanics and the conservation of energy. Additionally, there is a semantic debate regarding the classification of V(𝑥, 𝑑𝑥) as a potential. The thread emphasizes the importance of understanding the mathematical framework behind conservative forces in physics.
Kashmir
Messages
466
Reaction score
74
Goldstein writes

"only if ##V## is not an explicit function of time is the system conservative"That means ##V(r,\dot{r})## is a conservative potential, however I think that only potentials of the form ##V(r)## are conservative potentials.

Could you please tell me where I'm going wrong.

Thank you.
 
Physics news on Phys.org
PeroK said:
There's a discussion here about whether the magnetic force is conservative or not.

https://en.wikipedia.org/wiki/Conservative_force

And, there is plenty of further discussion online.
If we define a conservative force those whose closed loop integral is zero, then ##V(r,\dot{r})## isn't conservative?
That's the definition the author began with.
 
Kashmir said:
If we define a conservative force those whose closed loop integral is zero, then ##V(r,\dot{r})## isn't conservative?
That's the definition the author began with.
I'm not familiar with Goldstein, so I'm not sure what he's up to!
 
I'd not call ##V(\vec{x},\dot{\vec{x}})## a potential, but that's only a semantic question.

The math simply is that the first variation of the action is invariant under time translations if the Lagrangian is not explicitly time dependent, and then the Hamilotonian,
$$H=\dot{q}^k p_k - L=\text{const}$$
along the solutions of the Euler-Lagrange equations of motion, where the canonical momenta are defined by
$$p_k=\frac{\partial L}{\partial \dot{q}^k}.$$
 
The rope is tied into the person (the load of 200 pounds) and the rope goes up from the person to a fixed pulley and back down to his hands. He hauls the rope to suspend himself in the air. What is the mechanical advantage of the system? The person will indeed only have to lift half of his body weight (roughly 100 pounds) because he now lessened the load by that same amount. This APPEARS to be a 2:1 because he can hold himself with half the force, but my question is: is that mechanical...
Some physics textbook writer told me that Newton's first law applies only on bodies that feel no interactions at all. He said that if a body is on rest or moves in constant velocity, there is no external force acting on it. But I have heard another form of the law that says the net force acting on a body must be zero. This means there is interactions involved after all. So which one is correct?
Thread 'Beam on an inclined plane'
Hello! I have a question regarding a beam on an inclined plane. I was considering a beam resting on two supports attached to an inclined plane. I was almost sure that the lower support must be more loaded. My imagination about this problem is shown in the picture below. Here is how I wrote the condition of equilibrium forces: $$ \begin{cases} F_{g\parallel}=F_{t1}+F_{t2}, \\ F_{g\perp}=F_{r1}+F_{r2} \end{cases}. $$ On the other hand...
Back
Top