Symbolic Representation of General Alternating Waves and of Double Frequency Vector Products.pdf
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Symbolic Representation of General Alternating Waves and of Double Frequency Vector Products
A payerfresented at the Sixteenth General Meet-
ing of the A merican Institute of Electrical
Engineers, Boston, June 26th, z899, President
Kennelly in the Chair.
SYMBOLIC REPRESENTATION OF GENERAL AL-
TERNATING WAVES AND OF DOUBLE
FREQUENCY VECTOR PRODUCTS.
BY CHARLES PROTEUS STEINMETZ.
PART 1.
a. Graphically alternating currents and E. M. F.s are usually
represelnted by vectors. A vector is a quantity having length
and direction. The length represents the intensity, the direction
the phase of the alternating wave. The vectors generally issue
from the center of co-ordinates.
In the topographical method, however, which is more conven-
ient for complex nietworks, as interlinked polyphase circuits, the
alternating wave is represented by the straight line between two
points, these points representing the absolute values of potential
(with regard to anv reference point chosen as co-ordinate center)
and their connection the difference of potential, in phase and in-
tensity. Algebraically these vectors are represented by complex
quantities. The impedance, admittance, etc., of the circuit is a
complex quantity also, In symbolic denotation.
Thus current, E. M. F.S impedanee and admittance are related
by muultiplication and division of complex quantities similar as
current, E. M. F., resistance and conductance are related by
Ohms law in direct current circuiits.
In direct current circuits, power is the product of current into
E. M. F. In alternating current circuits, if .
E= +jei
269
Authorized licensed use limited to: NATIONAL LIBRARY OF CHINA. Downloaded on March 12,2010 at 06:08:38 EST from IEEE Xplore. Restrictions apply.
270 STEINMJETZ ON SYMBOLlC REPRESEFNTATION LJune 26,
The product:
Po0= El (el i ell ill) +± (ell1 + elIt11)
is not the power, that is multiplication and divisioni which are
correct in the inter-relatioll of current, E. M. F., impedance, do
not give a correct result in the inter-relatiorn of E. M. F., current
power. The reason is that E I are vectors of
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