Albert Einstein's On The Electrodynamics Of Moving Bodies

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In Albert Einstein’s 1905 paper entitled On the Electrodynamics of Moving Bodies, he outlines his argument for what understand today as special relativity, which stems from the two aforementioned postulates. The problem begins with the applications of Maxwell’s equations for the static and nonstatic cases. While Maxwell’s equations are symmetric for stationary bodies, asymmetries arise in the electrodynamic equations. Looking at the example of motion in a magnet and a conductor, Einstein explains that the equations depend only on the relative motion between the two (1). Whereas the previous models heavily depended on which component was moving. The ether model, disproved in the 1887 Michelson-Morley experiment along with the previously mentioned magnet/conductor setup, suggests that “the phenomena of electrodynamics as well as of mechanics possess no properties corresponding to the idea of absolute rest” (Einstein, On the Electrodynamics of Moving Bodies 1). Furthermore, Einstein postulates that the laws of physics (he specifically mentions electrodynamics and optics) are the same in any frame of reference. This is what he calls the “Principle of Relativity.” He also postulates that light in vacuum will always propagate with velocity c, regardless of the motion of the reference frame. He abandons the idea of the luminous ether here because ether necessitates the absolute rest that Einstein argues against. Einstein establishes an inertial reference, where Newton’s laws hold. He calls this the “stationary frame.” He defines the position through standard Euclidean geometry using Cartesian coordinates. Motion is defined as the change in the coordinates according to the time. But what do we mean by time? He proposes a thought experimen... ... middle of paper ... ...eory of Relativity). Through this paper, Einstein expands on his ideas in Special Relativity and incorporates acceleration into his argument to include the gravitational force. The gravity that he proposes in this expanded paper is radically different from Newton’s idea of gravity. One concept that is notably absent in Einstein’s paper on Special Relativity is the famous equation: E=mc^2. This equation appears in a paper response to The Electrodynamics of Moving Bodies entitled, Does the Inertia of a Body Depend Upon Its Energy-Content? The ultimate conclusion of this paper was that “the mass of a body is a measure of its energy-content changes by L, the mass changes in the same sense by L/9 × 1020” (3). The equation we know as E=mc^2 appear in a different form as: K_0-K_1=1/2 L/C^2 v^2. Here the energy measurement of L is measured in ergs (1 erg = 10-7 Joules).

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