An introduction to the mathematical theory of attraction ...

2 lIntroductory. As regards their mutual action, charges of electricity behave therefore to a certain extent like masses of gravitating matter, but there is an important difference which is immediately manifested. In the case of gravitating matter, the mutual force between two particles is always attractive; but charges of electricity, on the other hand, sometimes attract and sometimes repel one another. The observed phenomena can be explained by supposing that an electric charge, or in common language electricity, is one or other of two different kinds; that two charges or quantities of electricity of the same kind repel one another; and that two charges of opposite kinds attract one another, the force in each case being proportional to the product of the charges or quantities of electricity. To express mathematically what has been said above, we must regard one kind of electricity as positive and the other kind as negative. A quantity of electricity which occupies a space so small that it may be regarded as a point may be called an electric particle; and if a force which is repulsive be considered as positive, we may enunciate the fundamental law of electric forces by saying, that two particles of electricity act on each other with a force directly proportional to the proclct of their masses, and inversely proportional t the square of the distance between them. The word ' mass ' is here used only in reference to the amount of bfrce which the corresponding quantity of electricity is capable of producing, and is not meant to imply inertia or exclusive occupation of space. Looked at from a mathematical point of view, electric forces are of a more general character than those resulting from gravitation, and the study of the former includes that of the latter. 3. Distribution of Electricity.-As the electric forces due to the elements of an electrified body have each a definite magnitude, and pass through the elements to which they correspond, it may be said that there is a certain quantity of electricity accumulated in each space-element of the body, and we may consider the distribution of electricity in an electrified conductor. 4. Magnetic Forces.-The elementary forces due to the presence of a magnetized body are in some respects

/ 309
Pages

Actions

file_download Download Options Download this page PDF - Pages 2-21 Image - Page 2 Plain Text - Page 2

About this Item

Title
An introduction to the mathematical theory of attraction ...
Author
Tarleton, Francis Alexander.
Canvas
Page 2
Publication
London:: Longmans, Green & Co.,
1899-1913.
Subject terms
Attractions

Technical Details

Link to this Item
https://name.umdl.umich.edu/abr3212.0001.001
Link to this scan
https://quod.lib.umich.edu/u/umhistmath/abr3212.0001.001/21

Rights and Permissions

The University of Michigan Library provides access to these materials for educational and research purposes. These materials are in the public domain in the United States. If you have questions about the collection, please contact Historical Mathematics Digital Collection Help at [email protected]. If you have concerns about the inclusion of an item in this collection, please contact Library Information Technology at [email protected].

DPLA Rights Statement: No Copyright - United States

Manifest
https://quod.lib.umich.edu/cgi/t/text/api/manifest/umhistmath:abr3212.0001.001

Cite this Item

Full citation
"An introduction to the mathematical theory of attraction ..." In the digital collection University of Michigan Historical Math Collection. https://name.umdl.umich.edu/abr3212.0001.001. University of Michigan Library Digital Collections. Accessed June 20, 2025.
Do you have questions about this content? Need to report a problem? Please contact us.