Theory of Electricity And Magnetism
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In our eReader you can find the full English version of the book. Read Theory of Electricity And Magnetism Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Theory of Electricity And Magnetism
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289 for the given system. From the slow variation of the k's it follows that they can be regarded as constant during a considerable lapse of time and thus the motion itself as approximately cyclic (during that period). After a greater lapse of time the parameters k will assume other values, and the motion can again be regarded as cyclic. We can, therefore, define a cycle as a system containing only cyclic and slowly changing coordinates or parameters. By equation (2) our general equations of mo...tion (1) for cycles reduce to where L and K denote the forces that tend to increase the cyclic coordinates I and the parameters k respectively. The simplest case of cyclic motion is where we have a single cyclic coordinate I ; such a system is called a monocycle. The positions of all parts of such a system, except those due to the slow variation of the parameters k, will then be determined by the position of a single driving-point defined by that coordinate. If the driving- point is at rest, all parts of the system will remain at rest, whereas, if it is moving with a given velocity I', the motions of all its masses will be determined by that velocity.
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To quickly assess the difficulty of the text, read a short excerpt:
289 for the given system. From the slow variation of the k's it follows that they can be regarded as constant during a considerable lapse of time and thus the motion itself as approximately cyclic (during that period). After a greater lapse of time the parameters k will assume other values, and the motion can again be regarded as cyclic. We can, therefore, define a cycle as a system containing only cyclic and slowly changing coordinates or parameters. By equation (2) our general equations of mo...tion (1) for cycles reduce to where L and K denote the forces that tend to increase the cyclic coordinates I and the parameters k respectively. The simplest case of cyclic motion is where we have a single cyclic coordinate I ; such a system is called a monocycle. The positions of all parts of such a system, except those due to the slow variation of the parameters k, will then be determined by the position of a single driving-point defined by that coordinate. If the driving- point is at rest, all parts of the system will remain at rest, whereas, if it is moving with a given velocity I', the motions of all its masses will be determined by that velocity.
What to read after Theory of Electricity And Magnetism?
You can find similar books in the "Read Also" column, or choose other free books by Charles Emerson Curry to read onlineMoreLess
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