Lorentz invariance of wave eqn.

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SUMMARY

The classical wave equation is Lorentz invariant, as demonstrated through the application of the Lorentz transformation. The equation is expressed as (c² ∂²/∂t² + ∂²/∂x² + ∂²/∂y² + ∂²/∂z²) φ = 0. The transformation involves substituting derivatives with respect to the transformed coordinates, ensuring that the wave equation retains its form under Lorentz transformations. Proper application of the chain rule is crucial for this proof.

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  • Understanding of the classical wave equation
  • Familiarity with Lorentz transformations
  • Knowledge of partial derivatives
  • Basic principles of special relativity
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  • Study the derivation of Lorentz transformations in detail
  • Learn about the implications of Lorentz invariance in physics
  • Explore the mathematical properties of partial differential equations
  • Investigate the role of the chain rule in multivariable calculus
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Students of physics, particularly those studying special relativity, as well as educators and researchers interested in the mathematical foundations of wave equations.

Hymne
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Hello! Hopefully somebody could give me a push from behind on this one :)

Homework Statement



Show that the classical wave equation is lorentz invariant.

The Attempt at a Solution


I tried to exchange all derivatives by the chain rule:

(c^2 \frac{d^2 }{dt^2} + \frac{d^2 }{dx^2} + \frac{d^2 }{dy^2} + \frac{d^2 }{dz^2}) \phi = 0 ; \quad<br /> <br /> \frac{d}{dx} \rightarrow \frac{d}{dx}\frac{dx}{dx&#039;}
And the same for the time derivative and use lorentz transformation. But somewhere it goes wrong..
 
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I'd just substitute in the transformed coordinates and boil it all back down to what it started as. Not sure I'd use the chain rule explicitly.

Adrian.
 

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