178 ELECTRICAL APPARATUS ill, II > li . MS 4 'V 105. Let, in a general alternating-current transformer : secondary " — -- ~ J_. s = ratio primary , ,, ,. „ frequency, or slip ; H J' * thus, if: / = primary frequency, or frequency of impressed e.m.f., sf = secondary frequency; and the e.m.f. generated per secondary turn by the mutual flux has to the e.m.f. generated per primary turn the ratio, s, s = 0 represents synchronous motion of the secondary; s < 0 represents motion above synchronism—driven by external mechanical power, as will be seen; s = I represents standstill; s > I represents backward motion of the secondary, that is, motion against the mechanical force acting between primary and secondary (thus representing driving by external mechanical power). Let: n0 = number of primary turns in series per circuit; HI = number of secondary turns in series per circuit; a = ~ = ratio of turns ; Y = g — jb = primary exciting admittance per circuit; where: where: where: g = effective conductance; 6 = susceptance; ZQ = r0 +• j#o = internal primary self-inductive impedance per circuit, rQ = effective resistance of primary circuit; XQ = self-inductive reactance of primary circuit; n = TI + >jxi — internal secondary self-inductive im- pedance per circuit at standstill, or for s ~ 1, 7*1 = effective resistance of secondary coil; Xi = self-inductive reactance of secondary coil at stand- still, or full frequency, s = 1,