The time-independentKlein-Gordon equation reduces to one version of it, which has an extra lambda-squared term subtractedfrom one side.
For an incompressible flow, one method of solving the Navier-Stokes equation involves taking thedivergence of the momentum terms to find a "pressure" version of this equation. The time-independentKlein-Gordon equation reduces to one version of it, which has an extra lambda-squared term subtractedfrom one side. Solutions to that modification of this equation are sums of Yukawa potentials. An exponentialterm is added to one side of this equation in an extension commonly used to model solvation; that extension isco-named for (*) Boltzmann. For gravity, one side of this equation is four pi G rho, and this equation is commonlysolved using the method of images. For 10 points, name this equation which states that negative free-charge densityequals del squared of the potential, the inhomogeneous version of Laplace's equation.
For an incompressible flow, one method of solving the Navier-Stokes equation involves taking thedivergence of the momentum terms to find a "pressure" version of this equation.
Poisson equation