circuit, with three corners 1, 2, 3 assumed to be accessible, and the fourth inaccessible, or concealed. Generalizing, we have the following definition:
The direct capacities of an electrical system with n given accessible terminals are defined as the n(n - 1)/2 capacities which, connected between each pair of terminals, will be the exact equivalent of the system in its external reaction upon any other electrical system with which it is associated only by conductive connections through the accessible terminals.
An image should appear at this position in the text. To use the entire page scan as a placeholder, edit this page and replace "{{missing image}}" with "{{raw image|The Bell System Technical Journal, Volume 1, 1922.pdf/20}}". Otherwise, if you are able to provide the image then please do so. For guidance, see Wikisource:Image guidelines and Help:Adding images. |  |
Fig. 1—Equivalent Direct Capacities. G4 = C14 + C24 + C24 = Grounded Capacity of Branch-Point 4
The total direct capacity between any group of the terminal and all of the remaining accessible terminals, connected together, is called the grounded capacity of the group.
This definition of direct capacity presents the complete set of direct capacities as constituting an exact, symmetrical, realizable physical substitute for the given electrical system for all purposes, including practical applications. Direct capacities are Maxwell's "coefficients of mutual induction," but with the sign reversed, their number being increased so as to include a direct capacity between each pair of terminals.
In considering direct capacities we exclude any direct coupling, either magnetic or electric, from without with the interior or the electrical system, since we have no concern with its internal structure; we are restricted to its accessible, peripheral points or terminals; some care has been taken to emphasize this in the wording of the definition.
