The Dynamics of Particles And of Rigid, Elastic, And Fluid Bodies: Being ...
The Dynamics of Particles And of Rigid, Elastic, And Fluid Bodies: Being ...
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In our eReader you can find the full English version of the book. Read The Dynamics of Particles And of Rigid, Elastic, And Fluid Bodies: Being ... 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 The Dynamics of Particles And of Rigid, Elastic, And Fluid Bodies: Being ...
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der Phjs. n. Chem. S6, p. 177, 1898.
Digitized by VjOOQIC 12S, 1*4, 125] CHARACTERISTICS OF POTENTIAL, 363 2^. Its first partial derivatiTes are eYerrwhere holomorphic 3*^. Its second deriTatives are finite.
4*^. V yanishes at infinity to the first order, Urn (JRF) = 3f ; >j-> 0-' s~ vanish to second order.
Ox dy OS ' y b^. V satisfies everywhere Poisson's differential equation lim(i?|^) = -3fcos^.
d^^ + W^ '^' ^ " ^""^^ and outside of attracting matter, Laplace's equation c*V d*V d*V _ ^ Any f...unction having all these properties is a Newtonian potential function.
The field of force X, Y, Z is a solenoidal vector at all points outside of the attracting bodies, and hence if we construct tubes of force, the flux of force is constant through any cross -section of a given tube. A tube for which the flux is unity will be called a unit tube. The conception of lines of force and of tiie solenoidal property is due to Faraday.
Since F is a harmonic function outside of the attracting bodies, it has neither maximum nor minimum in free space, but its maximum and minimum must lie within the attracting bodies or at infinity.
What to read after The Dynamics of Particles And of Rigid, Elastic, And Fluid Bodies: Being ...?
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:
der Phjs. n. Chem. S6, p. 177, 1898.
Digitized by VjOOQIC 12S, 1*4, 125] CHARACTERISTICS OF POTENTIAL, 363 2^. Its first partial derivatiTes are eYerrwhere holomorphic 3*^. Its second deriTatives are finite.
4*^. V yanishes at infinity to the first order, Urn (JRF) = 3f ; >j-> 0-' s~ vanish to second order.
Ox dy OS ' y b^. V satisfies everywhere Poisson's differential equation lim(i?|^) = -3fcos^.
d^^ + W^ '^' ^ " ^""^^ and outside of attracting matter, Laplace's equation c*V d*V d*V _ ^ Any f...unction having all these properties is a Newtonian potential function.
The field of force X, Y, Z is a solenoidal vector at all points outside of the attracting bodies, and hence if we construct tubes of force, the flux of force is constant through any cross -section of a given tube. A tube for which the flux is unity will be called a unit tube. The conception of lines of force and of tiie solenoidal property is due to Faraday.
Since F is a harmonic function outside of the attracting bodies, it has neither maximum nor minimum in free space, but its maximum and minimum must lie within the attracting bodies or at infinity.
What to read after The Dynamics of Particles And of Rigid, Elastic, And Fluid Bodies: Being ...?
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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