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  2. Jefimenko's equations - Wikipedia

    en.wikipedia.org/wiki/Jefimenko's_equations

    The Heaviside–Feynman formula, also known as the Jefimenko–Feynman formula, can be seen as the point-like electric charge version of Jefimenko's equations. Actually, it can be (non trivially) deduced from them using Dirac functions, or using the Liénard-Wiechert potentials. [4] It is mostly known from The Feynman Lectures on Physics, where ...

  3. File:Explanation of variables in Heaviside-Feynman formula.svg

    en.wikipedia.org/wiki/File:Explanation_of...

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  4. List of unsolved problems in chemistry - Wikipedia

    en.wikipedia.org/wiki/List_of_unsolved_problems...

    This is a list of unsolved problems in chemistry. Problems in chemistry are considered unsolved when an expert in the field considers it unsolved or when several experts in the field disagree about a solution to a problem.

  5. Propagator - Wikipedia

    en.wikipedia.org/wiki/Propagator

    These prescriptions are known as Feynman rules. Internal lines correspond to virtual particles. Since the propagator does not vanish for combinations of energy and momentum disallowed by the classical equations of motion, we say that the virtual particles are allowed to be off shell. In fact, since the propagator is obtained by inverting the ...

  6. Oliver Heaviside - Wikipedia

    en.wikipedia.org/wiki/Oliver_Heaviside

    Oliver Heaviside (/ ˈ h ɛ v i s aɪ d /, HEH-vee-syde; 18 May 1850 – 3 February 1925) was an English mathematician and physicist who invented a new technique for solving differential equations (equivalent to the Laplace transform), independently developed vector calculus, and rewrote Maxwell's equations in the form commonly used today.

  7. Green's function - Wikipedia

    en.wikipedia.org/wiki/Green's_function

    Then, the Heaviside step function Θ(x − x 0) is a Green's function of L at x 0. Let n = 2 and let the subset be the quarter-plane {(x, y) : x, y ≥ 0} and L be the Laplacian. Also, assume a Dirichlet boundary condition is imposed at x = 0 and a Neumann boundary condition is imposed at y = 0.

  8. Heaviside–Lorentz units - Wikipedia

    en.wikipedia.org/wiki/Heaviside–Lorentz_units

    To convert any formula between the SI, Heaviside–Lorentz system or Gaussian system, the corresponding expressions shown in the table below can be equated and hence substituted for each other. Replace 1 / c 2 {\displaystyle 1/c^{2}} by ε 0 μ 0 {\displaystyle \varepsilon _{0}\mu _{0}} or vice versa.

  9. Operational calculus - Wikipedia

    en.wikipedia.org/wiki/Operational_calculus

    Heaviside went further and defined fractional power of p, thus establishing a connection between operational calculus and fractional calculus. Using the Taylor expansion , one can also verify the Lagrange–Boole translation formula , e a p f ( t ) = f ( t + a ) , so the operational calculus is also applicable to finite- difference equations ...