The Theory of Electricity And Magnetism Being Lectures On Mathematical Physics
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It appeared that no experimenter ventured to attack the problem, it being evidently considered too difficult. The finite relaxation-time was determined for so good a conductor as water in some remarkable experiments by Cohn and AronsJ, who are entitled to the credit of discovering the finiteness of T for conductors.
* Cohn, Wied. Ann. 40, p. 625, 1890. T Elihu Thomson Prize, Electrician, 1892.
J Cohn u. Arons. "Leitungsvermb'gen und Dielektricitatsconstante. " Wied. Ann. 28, p. 454, 1886.
400 E...LECTKOKINETICS. [PT. II. CH. X.
207. Method of Cohn and Arons. Consider a condenser A, which may or may not be connected in parallel with the con- denser B and the resistance wire R. Let the capacity of A be K, the inductivity of the dielectric p. Let the conductivity of the dielectric in A be X and in B zero. Then the charge of one of the plates 1 of A is in terms of the induction, 182 (16), (8) ej = 7- 1 1 ( cos (nx) + g) cos (ny) + 3 cos (nz)) dS.
8 t On the other hand the quantity flowing through the dielectric in the condenser in unit time is (9) .
What to read after The Theory of Electricity And Magnetism Being Lectures On Mathematical Physics?
You can find similar books in the "Read Also" column, or choose other free books by Webster, Arthur Gordon, 1863-1923 to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
It appeared that no experimenter ventured to attack the problem, it being evidently considered too difficult. The finite relaxation-time was determined for so good a conductor as water in some remarkable experiments by Cohn and AronsJ, who are entitled to the credit of discovering the finiteness of T for conductors.
* Cohn, Wied. Ann. 40, p. 625, 1890. T Elihu Thomson Prize, Electrician, 1892.
J Cohn u. Arons. "Leitungsvermb'gen und Dielektricitatsconstante. " Wied. Ann. 28, p. 454, 1886.
400 E...LECTKOKINETICS. [PT. II. CH. X.
207. Method of Cohn and Arons. Consider a condenser A, which may or may not be connected in parallel with the con- denser B and the resistance wire R. Let the capacity of A be K, the inductivity of the dielectric p. Let the conductivity of the dielectric in A be X and in B zero. Then the charge of one of the plates 1 of A is in terms of the induction, 182 (16), (8) ej = 7- 1 1 ( cos (nx) + g) cos (ny) + 3 cos (nz)) dS.
8 t On the other hand the quantity flowing through the dielectric in the condenser in unit time is (9) .
What to read after The Theory of Electricity And Magnetism Being Lectures On Mathematical Physics?
You can find similar books in the "Read Also" column, or choose other free books by Webster, Arthur Gordon, 1863-1923 to read onlineMoreLess
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