Conserved quantities in mechanics

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The discussion centers on conserved quantities in classical dynamics, identifying energy, angular momentum, and momentum as primary conserved quantities, totaling seven distinct forms. The conversation raises the question of whether additional conserved quantities exist, suggesting that conservation laws stem from the invariance of the Lagrangian with respect to each degree of freedom. It emphasizes that while momentum is conserved in closed systems, the conditions must be specified, as mechanics is not limited to such systems. An example involving a hosepipe directed at a wall illustrates that momentum conservation holds true, even when considering the wall's reaction. Ultimately, the discussion highlights the importance of understanding the conditions under which these conservation laws apply.
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So having been through translation and rotation I can conclude that my book has found 3 conserved quantities in classical dynamics:
Energy
Angular momentum
Momentum
That is 7 separate quantities which are conserved E,Lx,Ly,Lz,px,py,pz
But this question is bothering me: How do we know that there are not more conserved quantities?
 
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Conservation laws come from invariance of the Lagrangian with each degree of freedom.
If you can think of another degree of freedom you can have another conservation law.
 
Is momentum always conserved?

Suppose I direct a hosepipe horizontally at a wall.

Please explain conservation of horizontal momentum at the wall face in this case.
 
Studiot said:
Is momentum always conserved?
In closed systems.

Some systems have additional conserved quantities, for example the Kepler problem or harmonic oscillators. But in the general case, you just have those 7 conserved quantities.
 
@mfb
Yes it is good to specify the conditions.
These were not originally specified and mechanics is not exclusively about closed systems, and should not be taught or thought of as such.

In my career I have seen spectacular failures of mechanical systems due to failure to appreciate this.
 
Studiot said:
Is momentum always conserved?

Suppose I direct a hosepipe horizontally at a wall.

Please explain conservation of horizontal momentum at the wall face in this case.
Simple. The (effectively) infinitely massive wall moves at an (effectively) infinitesimally small rate. The product mass*velocity is some finite, non-zero quantity that exactly obeys conservation of momentum.
 
So where does the perpendicular (to the flow) momentum come from at the wall face?
 
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