Lagrange with Higher Derivatives (Ostrogradsky instability)

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SUMMARY

The discussion centers on the implications of including higher derivatives, specifically ##\ddot{q_i}##, in a Lagrangian, leading to potential instability characterized by unbounded energy from below. The integral for energy conservation in such systems is presented as $$H(q,\dot q,\ddot q,\dddot q)=-L+2\frac{\partial L}{\partial \ddot q}\ddot q+\frac{\partial L}{\partial \dot q}\dot q-\frac{d}{dt}\Big(\frac{\partial L}{\partial \ddot q}\dot q\Big)$$, assuming ##L## is independent of time. The discussion highlights the Abraham-Lorentz-Dirac equation as a notable example, illustrating the causality issues and "run-away solutions" that arise, while confirming that energy conservation remains applicable despite these challenges.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with higher-order derivatives in physics
  • Knowledge of energy conservation principles in classical mechanics
  • Basic grasp of the Abraham-Lorentz-Dirac equation
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  • Study the implications of higher derivatives in Lagrangian mechanics
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Physicists, particularly those specializing in classical mechanics and field theory, as well as students exploring advanced topics in Lagrangian dynamics and stability analysis.

Arman777
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In class our teacher told us that, if a Lagrangian contain ##\ddot{q_i}## (i.e., ##L(q_i, \dot{q_i}, \ddot{q_i}, t)##) the energy will be unbounded from below and it can take any lower values (in other words be unstable). In this type of systems can we show that the energy is conserved ? Or in such system does energy conservation is applicable ?
 
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there must be some conservation law which follows from the time shift invariance of such systems; I would try to derive it first.

If I did not make an error the "energy" integral is as follows
$$H(q,\dot q,\ddot q,\dddot q)=-L+2\frac{\partial L}{\partial \ddot q}\ddot q+\frac{\partial L}{\partial \dot q}\dot q-\frac{d}{dt}\Big(\frac{\partial L}{\partial \ddot q}\dot q\Big)$$
This is under the assumption that ##L## does not depend on t surely.

Instability arises due to the last term I guess. This term is linear in ##\dddot q##
 
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Indeed, the most famous example is the Abraham-Lorentz-Dirac equation for a point particle moving in an external electromagnetic field including the radiation reaction, i.e., the backreaction on the motion of the particle by its own (radiation) field. It leads to serious problems with causality and "run-away solutions".
 
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So the energy conservation is applicable.
 

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