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For example for an isolated system the energy $E$ is conserved. But then any function of energy, (like $E^2,\sin E,\frac{ln|E|}{E^{42}}$ e.t.c.) is conserved too. Therefore one can make up infinitely many conserved quantities just by using the conservation of energy.

Why then one can usually hear of "system having N constants of motion"? "System having only one constant of motion"?

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Gotta run, so just a quick comment for now. There is an implicit notion of independence. If you can express one of the constants as the function of others then it's dependent. E.g. when working on a symplectic manifold, this means that flows (vector fields that correspond to the conserved quantities) span an $N$-dimensional vector space at every point. I.e. they form a $N$-plane distribution. –  Marek Feb 21 '11 at 11:39
    
aw, @Marek, you couldn't have made that a quick answer? –  David Z Feb 21 '11 at 23:57
    
@David: nah, because it's not a complete answer, so it doesn't feel right for me. For one thing it talks only about classical mechanics. There's more to add also about quantum mechanics (and relation to mutually compatible observables), etc. I'll try to give a more complete answer later. –  Marek Feb 22 '11 at 8:19
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The notion of (in)dependence has already been explained by Marek above. So out of all functions f(E), you should only pick one. I would just add that in many-body systems you usually require that the conserved charge be additive (for the sake of the thermodynamic limit). This selects E itself or its multiple. –  Tomáš Brauner Feb 22 '11 at 11:54
    
@Marek: +1 for comment; please make into an actual answer soon! –  genneth Feb 22 '11 at 16:18
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4 Answers

Maybe it is worth distinguishing independent integrals of motion from functions of integrals of motion? See equations (2) and (3) in my post. The number of independent constants of motion is limited with the number of independent initial data (if the problem is well posed).

EDIT: another way to understand it is to count independent degrees of freedom of the system.

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A system having N constants of motion means having N fundamental, mathematically derived quantities that are constant for the motion. $F = m dv/dt$ is physically derived from experiment. You can create the mathematically derived quantity work by forming the scalar product of both sides with a differential displacement:

$F\cdot dl = m dv/dt \cdot dl = m v \cdot dv$

Integrating over conservative forces, you get a constant of motion, kinetic energy + potential energy = constant. You can create another mathematically derived quantity impulse by multiplying both sides by dt:

$F dt = m dv/dt dt = m dv$

Integrating over a system where all the forces are internal and action = reaction, you get another constant of motion, total momentum = constant.

Look in any standard text book for the details of the above derivations, and Noether’s theorem which is another way of deriving constants of motion from physically derived quantities. The important point is they’re fundamental, mathematically derived constants of motion from physically derived quantities.

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Let us assume (for simplicity in this question) that the Hamiltonian H is time independent. Then any function f whose Poisson Bracket with H {f, H}=0 is a constant of motion. Also Poisson's Theorem is that if f,g are both constants of motion then so is {f,g} generating yet more constants of motion.

The clarification is that the functions f, g here define canonical changes of variable, so we are only interested in ones that replace the $p_i$ and $q_i$ with new coordinates $(P_i,Q_i)$. There are only going to be at most 2N of these.

The ideal arrangement is to cause as many of the $Q_i$'s as possible to drop out of the (transformed) Hamiltonian $H=H(P_i,Q_i)$, there only being N maximum available. So yes many "constants of motion" will be functions of one another (akin to having not only x(q),y(p) available as coordinates, but also x+y, $x^2$, etc), but one wants to use only those which lead to a simpler Hamiltonian.

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There are seven fundamental additive constants of the motion in classical mechanics, these are the energy and the three components of momentum and angular momentum. In other words, every constant of the motion, $C$, can be written uniquely as:

$\hspace{3cm} C=a_1E+a_2P_x+a_3P_y+a_4P_z+a_5L_x+a_5L_y+a_7L_z$

A proof of this fact can be found in Landau, Vol 1.

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