Title :
Analysis of bundle losses in high speed machines
Author :
Reddy, Patel B. ; Jahns, T.M.
Author_Institution :
Dept. of Electr. & Comput. Eng., Univ. of Wisconsin, Madison, WI, USA
Abstract :
Elevated frequencies in high-speed ac machines increase the skin effect in stator windings, making it necessary in many cases to divide each phase winding into high numbers of small-diameter strands connected in parallel. Unfortunately, circulating currents among the strands in a single bundle can significantly increase the total copper losses depending on several factors including the twisting (i.e., transposition) of the strands in the bundles. An analytical model for these bundle proximity losses is presented for individual bundles as well as slot-bound bundles configured for high-speed machines. Loss predictions provided by this model match well with finite element results for high-speed operation of a 55 kW (peak) PM machine with concentrated windings. Stators with litz and non-transposed windings are compared to highlight the large differences in their bundle proximity losses. Analytical and finite element results are shown to match well with experimental results at frequencies of 700 and 800 Hz.
Keywords :
AC machines; finite element analysis; losses; permanent magnet machines; skin effect; stators; PM machine; analytical model; bundle proximity losses; concentrated windings; copper losses; finite element results; frequency 700 Hz; frequency 800 Hz; high-speed AC machines; litz winding; loss predictions; nontransposed windings; power 55 kW; skin effect; slot-bound bundles; stator windings; AC machines; Analytical models; Finite element methods; Frequency; Machine windings; Predictive models; Proximity effect; Skin effect; Stator windings; Transformers; AC losses; ac machines; brushless machines; bundle losses; high efficiency; high speed; proximity losses;
Conference_Titel :
Power Electronics Conference (IPEC), 2010 International
Conference_Location :
Sapporo
Print_ISBN :
978-1-4244-5394-8
DOI :
10.1109/IPEC.2010.5542354