Undergrad Generalized Momentum is a linear functional of Velocity?

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SUMMARY

Generalized momentum is defined as a covariant quantity, while velocity is contravariant in the context of coordinate transformations on configuration space. The relationship between momentum and velocity is established through the equation P_a = M_{ab}(Q,t)\dot{Q}^b, where P_a is the generalized momentum derived from the Lagrangian \(\mathcal{L}(Q,\dot{Q},t)\). When the Lagrangian is quadratic in coordinate velocities, the generalized inertia tensor M_{ab} allows for a linear mapping of momentum as a functional of velocity. This relationship confirms that the contraction P_a\dot{Q}^a results in a scalar value.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with tangent and cotangent bundles
  • Knowledge of covariant and contravariant transformations
  • Basic concepts of functional analysis in physics
NEXT STEPS
  • Study the properties of tangent and cotangent bundles in differential geometry
  • Explore the implications of quadratic Lagrangians in classical mechanics
  • Learn about generalized inertia tensors and their applications
  • Investigate the role of scalar quantities in functional mappings
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Physicists, mechanical engineers, and students of advanced mechanics seeking to deepen their understanding of the relationship between generalized momentum and velocity in Lagrangian systems.

chmodfree
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Generalized momentum is covariant while velocity is contravariant in coordinate transformation on configuration space, thus they are defined in the tangent bundle and cotangent bundle respectively.
Question: Is that means the momentum is a linear functional of velocity? If so, the way to construct this functional?
 
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If the Lagrangian is quadratic in the coordinate velocities then it is linear at the point of the tangent bundle and can thus be expressed as the result of a linear mapping by a generalized inertia tensor, P_a = M_{ab}(Q,t)\dot{Q}^b

P_a = \frac{\partial \mathcal{L}(Q,\dot{Q},t)}{\partial \dot{Q}^a} = M_{ab}\dot{Q}^b with M not depending on any \dot{Q} if and only if the Lagrangian was quadratic in these velocities.
 
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jambaugh said:
If the Lagrangian is quadratic in the coordinate velocities then it is linear at the point of the tangent bundle and can thus be expressed as the result of a linear mapping by a generalized inertia tensor, P_a = M_{ab}(Q,t)\dot{Q}^b

P_a = \frac{\partial \mathcal{L}(Q,\dot{Q},t)}{\partial \dot{Q}^a} = M_{ab}\dot{Q}^b with M not depending on any \dot{Q} if and only if the Lagrangian was quadratic in these velocities.
Oh I see, that means the contraction P_a\dot{Q}^a is a real.
 
chmodfree said:
Oh I see, that means the contraction P_a\dot{Q}^a is a real.
I don't know about real... I imagine someone might cook up a Lagrangian with complex inertia, but the contraction is a scalar.
 
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jambaugh said:
I don't know about real... I imagine someone might cook up a Lagrangian with complex inertia, but the contraction is a scalar.
I mean it maps \dot{Q} from tangent bundle to the real number field as a functional... No problem now, thank you.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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