Elements of the Mathematical Theory of Electricity And Magnetism
Elements of the Mathematical Theory of Electricity And Magnetism
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In our eReader you can find the full English version of the book. Read Elements of the Mathematical 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 Elements of the Mathematical Theory of Electricity And Magnetism
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If the body at P is a small sphere of radius b, then since the elec- tric energy is equal to JS^F, it is in this case 1 (e ea 1 2 e \b~JPQ a or - n* 87, To find the surface density at a point S on the surface of the sphere, we must find the electric intensity along the normal.
88] ELECTRICAL IMAGES AND INVERSION 113 The electric intensity at S due to the charge e at P can by the triangle of forces be resolved into the two components e OS . () pa pg alon g ^ (ft) ~~ parallel to PO, while the ele...ctric intensity at S due to the charge ea/f at Q can be resolved into the components ea 1 OS (S) -^ parallel to PO.
Hence the components of the resultant intensity are a + y along the normal OS, and j8 + 8 parallel to PO.
Now the resultant intensity is along the normal, so that the component /? + 8 must vanish, and the resultant intensity along the normal is equal to a -h y, i. E. To JL _ a JLI PS 3 fQS*] e. OS e. OS or to ~~PQ3~ Since PS/QS is constant, the quantity inside the brackets is constant.
What to read after Elements of the Mathematical Theory of Electricity And Magnetism?
You can find similar books in the "Read Also" column, or choose other free books by J J Joseph John Thomson to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
If the body at P is a small sphere of radius b, then since the elec- tric energy is equal to JS^F, it is in this case 1 (e ea 1 2 e \b~JPQ a or - n* 87, To find the surface density at a point S on the surface of the sphere, we must find the electric intensity along the normal.
88] ELECTRICAL IMAGES AND INVERSION 113 The electric intensity at S due to the charge e at P can by the triangle of forces be resolved into the two components e OS . () pa pg alon g ^ (ft) ~~ parallel to PO, while the ele...ctric intensity at S due to the charge ea/f at Q can be resolved into the components ea 1 OS (S) -^ parallel to PO.
Hence the components of the resultant intensity are a + y along the normal OS, and j8 + 8 parallel to PO.
Now the resultant intensity is along the normal, so that the component /? + 8 must vanish, and the resultant intensity along the normal is equal to a -h y, i. E. To JL _ a JLI PS 3 fQS*] e. OS e. OS or to ~~PQ3~ Since PS/QS is constant, the quantity inside the brackets is constant.
What to read after Elements of the Mathematical Theory of Electricity And Magnetism?
You can find similar books in the "Read Also" column, or choose other free books by J J Joseph John Thomson to read onlineMoreLess
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