PHASE CONVERSION

217

the monocyclic quadrature voltage, $Q = CD, and current, J0.
Denoting then:

E = e = supply voltage, AB, and / = supply current, and
EI, jB2 = voltages, /i, JT2 = currents in the two sides of the
monocyclic square.

It is then, counting voltages and currents in the direction
indicated by the arrows in Fig. 67:

#2 + Ei = e,

hence:

2 '

and:

substituting:

into (3) gives:

(i)

(2)

(3)

(4)

substituting (2) into (5) gives:

(5)

(6)

substituting (6) into (2) gives:

IL.+Z')

F2 4- 2 I

_

+ Fz + 2

(7)