By Jacqueline B. Glasthal
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Extra resources for 5 Minute Daily Practice - Test Taking - Grades 4 - 8
Then we may write the mmf equation in complex notation as . I lwl ,; "'! I + . I 2w 2 = I owl (3-2) In our further discussion, the term "magnetizing current" will refer to the equivalent sinusoidal magnetizing current 1 0 , Now we are in a position to present the primary mmf i l w 1 as a sum of iOw l and (illVl - iolVl) = -i 2lV z which ba lances the secondary mmf i zlV 2 , and the magnetic flux in operation on load as a sum of t hree fluxes, namely: (a) the mutual magnetic flux
Ii) Structural Parts of a Transformer The fu nction of the structural parts in any transformer is to provide electrical insulation between the windings, to hold the core and coils in place, to cool the transformer, to provide connection between the transformer windings and the associated electric. li nes, and the like. and the other clamping and packing-on t parts may also be classed as structural parts. Ch. he structural parts, choosing all oil-immersed three-phase power tr ansformer as an example .
The r esultant r el at ionship between t he in st ant aneous va lues of the two quantities, cD = j (i o), is i dent ical Part One. , when eddy currents are nonexi stent. c. magnetization curve (or characteristic) of a tran sformer. It can be construc ted on the basis of Ampere's circuital la w in in t egral form . On aligning the loop enc losing t he current in all the primar y turns, iOw 1, with a line of for ce of t he mutual magnetic flux in the core, Ampere's circuital law ma y be written I iowt = I ~ Hzdl The procedure yielding the cir culation of the H vector is as follows: (1) Assign a desired va lue to the magnet ic flux in th e core .