Lagrange with Higher Derivatives (Ostrogradsky instability)

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Discussion Overview

The discussion centers on the implications of including higher derivatives in a Lagrangian, specifically regarding energy conservation and stability in systems described by such Lagrangians. The scope includes theoretical considerations and mathematical reasoning related to Lagrangian mechanics.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • One participant notes that including higher derivatives like ##\ddot{q_i}## in a Lagrangian can lead to unbounded energy from below, raising questions about energy conservation in such systems.
  • Another participant suggests that there may still be a conservation law due to time shift invariance, proposing to derive it based on the structure of the Hamiltonian derived from the Lagrangian.
  • A third participant references the Abraham-Lorentz-Dirac equation as a notable example of issues arising from higher derivatives, particularly concerning causality and the emergence of "run-away solutions."
  • One participant asserts that energy conservation is applicable in these systems, although the basis for this claim is not elaborated upon.

Areas of Agreement / Disagreement

There is disagreement regarding the applicability of energy conservation in systems with higher derivatives. While one participant asserts that energy conservation holds, others raise concerns about stability and causality, indicating that the discussion remains unresolved.

Contextual Notes

Participants have not fully resolved the implications of the last term in the Hamiltonian, which is linear in ##\dddot{q}##, and its role in the stability of the system. There are also assumptions about the Lagrangian's independence from time that have not been explicitly stated.

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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