Minkowski Force due to a quadratic in velocity potential

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SUMMARY

The discussion centers on deriving the Minkowski force from a generalized potential suitable for a covariant Lagrangian, specifically referencing Goldstein problem 9 from chapter 7. The potential is expressed as −Aλν(xμ)uλuν, where Aλν is a symmetric world tensor and u^v represents the components of world velocity. The Lagrangian is defined as (1/2)m*u_v*u^v minus U, leading to the formulation of the Lagrange equations of motion. The Minkowski force is identified as the derivative of four-momentum with respect to proper time, represented as dP/dτ.

PREREQUISITES
  • Understanding of covariant Lagrangian mechanics
  • Familiarity with four-vectors and four-velocity
  • Knowledge of Minkowski spacetime and relativistic dynamics
  • Proficiency in deriving equations of motion from Lagrangians
NEXT STEPS
  • Study the derivation of Lagrange equations from a covariant perspective
  • Learn about the properties of symmetric tensors in relativistic physics
  • Explore the concept of four-momentum and its applications in special relativity
  • Investigate the relationship between four-acceleration and Minkowski force
USEFUL FOR

This discussion is beneficial for physics students, particularly those studying classical mechanics and special relativity, as well as researchers focusing on relativistic dynamics and Lagrangian formulations.

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Homework Statement


A generalized potential suitable for use in a covariant Lagrangian for a single particle. This is Goldstein problem 9 chapter 7.

−Aλν(xμ)uλuν

where Aλν stands for a symmetric world tensor of the second rank and u^v are the components of the world velocity. If the Lagrangian is made up of (1/2)m*u_v*u^v minus U, obtain the Lagrange equations of motion. What is the Minkowski force? Give the components of the force as observed in some Lorentz frame.

Homework Equations



Euler equation of motion where the derivatives are taken with respect to the four velocity and where and the time part if the proper time. Also that the four force is the mass times the four velocity.

The Attempt at a Solution



When I workout the Lagrangian I have an extra term which is proportional to the four acceleration. My first thought is to solve for the four acceleration and then multiply it by the mass to get the Minkowski force. Is that valid? [/B]
 
Minkowski 4-Force = dP/d-tau where P is 4-momentum;
or 4-Force = gamma(3-Force, id/dt(mc)) where m is relativistic mass.
 

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