Angular Momentum, Problem from Landau Lifshitz

Click For Summary

Homework Help Overview

The discussion revolves around a problem from Landau Lifshitz concerning angular momentum and symmetries in mechanics. Participants are exploring the implications of symmetries in a physical system and how they relate to the conservation of angular momentum and momentum.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the significance of symmetries in the problem, particularly how they relate to the conservation laws of angular momentum and momentum. There are attempts to derive conditions under which these quantities remain constant, with references to the Lagrangian formalism.

Discussion Status

The discussion is ongoing, with participants offering insights into the nature of symmetries and their effects on the system. Some have suggested checking the formal derivation using the Lagrangian, while others are clarifying the conditions under which certain quantities remain constant. Multiple interpretations of the problem are being explored.

Contextual Notes

Participants are working under the constraints of the problem as presented in the textbook, which may involve specific assumptions about the nature of the fields and symmetries involved. There is an acknowledgment of the need for a deeper understanding of the motion that does not alter the Lagrangian.

Jimmy84
Messages
190
Reaction score
0
This is problem 3 from section 9 of Mechanics, Landau Lifgarbagez.
I have been trying to understand the problem but I have no idea how to solve it.

Can someone give me a hand please? any comment or suggestion is very welcome.

Thanks for your time.

Best regards.
 

Attachments

  • pppp.png
    pppp.png
    22.7 KB · Views: 677
  • pppp2.png
    pppp2.png
    33.5 KB · Views: 675
Physics news on Phys.org
It is all about something physicists are very fond of,ie,symmetries. For instance in a) you can not notice any displacement parallel to the plane either can you notice any rotation about an axis which is perpendicular to the plane. You must check doing the formal derivation working with the Lagrangian of the system.
 
Sorry for the bad english!

M is constant when the movement is parallel to the axis of simetry of the field
ie:

a) if the field is a plane xy--->symmetry z axis--->M_z=doesnt change

P is constant when the movement is in the "same field", in a) if the particle moves in any direction of x or y P is constant, the reason is because the vectors of the field are orientated in the direction of the axis of symetry (in case a) ), then P only change in that direction.

ie: b) the symetry is a cylinder, then Mz doesn't change in a Z-cylinder. But if you imagine the field, is like infinite cylinders, all parallel, then if you want the particle moves "in the same field", only the z-motion is the correct.
 
in case b) M_z=const. and P_z=const. I think a field compatible with cilindrical symetry mus be one that points in the radial direction perpendicular to z and it's magnitud depends only on the distance to the z axis.
However the key to this problem is understanding what kind o motion does not change the Lagrangian and this allows you to do it fomally(mathematically)
 

Similar threads

Replies
3
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 0 ·
Replies
0
Views
1K
  • · Replies 2 ·
Replies
2
Views
10K
Replies
1
Views
404
  • · Replies 1 ·
Replies
1
Views
2K
Replies
5
Views
1K
  • · Replies 17 ·
Replies
17
Views
1K
  • · Replies 5 ·
Replies
5
Views
2K