The 4-D Laplace equation and wave equation

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SUMMARY

The discussion centers on the relationship between the 4-D Laplace equation and the wave equation in the context of relativity. The scalar wave equation in a four-dimensional coordinate system (x,y,z,ict) is expressed as \(\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}+\frac{\partial^2\phi}{\partial (ict)^2}=0\). In contrast, the ordinary wave equation is given by \(\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}=\frac{1}{v^2}\frac{\partial^2\phi}{\partial t^2}\). The discussion concludes that in Minkowski spacetime, the wave equation can be represented using the D'Alembert operator \(\square \phi=0\), linking it to Nordstrom's first theory of gravitation.

PREREQUISITES
  • Understanding of the scalar wave equation in four-dimensional spacetime
  • Familiarity with the Laplace equation in three-dimensional classical mechanics
  • Knowledge of the D'Alembert operator and its application in relativity
  • Basic concepts of Minkowski spacetime and its signature
NEXT STEPS
  • Study the derivation and applications of the D'Alembert operator in physics
  • Explore the implications of Nordstrom's first theory of gravitation
  • Investigate the differences between classical wave equations and relativistic wave equations
  • Learn about the mathematical formulation of Minkowski spacetime and its significance in relativity
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Physicists, mathematicians, and students of theoretical physics interested in the interplay between wave equations and relativity, particularly those focusing on advanced concepts in spacetime and field theories.

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In relativity, the scalar wave equation in the coordinate system (x,y,z,ict)
is
\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}+\frac{\partial^2\phi}{\partial (ict)^2}=0

In 3D classical mechanics, the Laplace equation is:{when the coordinate system is (x,y,z)+t}
\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}=0

And the ordinary wave equation is
\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}=\frac{1}{v^2}\frac{\partial^2\phi}{\partial t^2}

the first equation is similar to the third,and the second equation has the same format of dimensions as the first.

So, does this mean that a wave equation in 4 dimensions is a 4-D laplace equation in relativity,or something else,Thx very much.
 
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pliu123123 said:
In relativity, the scalar wave equation in the coordinate system (x,y,z,ict)
is
\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}+\frac{\partial^2\phi}{\partial (ict)^2}=0

In 3D classical mechanics, the Laplace equation is:{when the coordinate system is (x,y,z)+t}
\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}=0

And the ordinary wave equation is
\frac{\partial^2\phi}{\partial x^2}+\frac{\partial^2\phi}{\partial y^2}+\frac{\partial^2\phi}{\partial z^2}=\frac{1}{v^2}\frac{\partial^2\phi}{\partial t^2}

the first equation is similar to the third,and the second equation has the same format of dimensions as the first.

So, does this mean that a wave equation in 4 dimensions is a 4-D laplace equation in relativity,or something else,Thx very much.

Yes! In four dimensional spacetime of Minkowski with signature (+,-,-,-), the wave equation is

\square \phi=0

with \square = {\partial}^2_t-{\nabla}^2 being the famous D'Alembert operator, which is of course the field equation of Nordstrom's first theory of gravitation!

AB
 

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