3 Phase-controlled DC motor drives

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• By combining armature and field control, awide range of speed control is possible.• The relationship between armature currentand torqueT e = Kφ f i a• The rated torqueT er = Kφ fr i ar• The normalized versionTenT=Teer=KφKφffriiaarφ= (φffri)(iaar)=φfnian,p.u.(perunit)
• Similarly, the air gap power isP an = e n i an , p.u.where e n is the normalized induced emf.•As i an is set to 1 p.u., the normalized air gappower becomesP an = e n , p.u.• The steady-state power output is kept fromexceeding its rated design value, which is 1p.u.
Page 1 and 2: 3 Phase-controlled DC motor drives
Page 3 and 4: • In field control, the applied a
Page 5: • Fig. 3.1
Page 9 and 10: 3.2.5 Four-quadrant operation• Du
Page 11 and 12: • Fig. 3.5 illustrates the speed
Page 13 and 14: • Two basic methods by using stat
Page 15 and 16: • The bridge conduction is delaye
Page 17 and 18: • In the case that the load curre
Page 19 and 20: • Fig. 3.10 is a three-phase thyr
Page 21 and 22: • A control technique to overcome
Page 23 and 24: Control modeling• The gain of the
Page 25 and 26: • Fig. 3.15 is current source con
Page 27 and 28: • Fig. 3.17 is a half-controlled
Page 29 and 30: • Fig. 3.20 shows the converter c
Page 31 and 32: • The normalized electromagnetic
Page 33 and 34: where ω s = 2πf s , β = tan -1 (
Page 35 and 36: • Fig 3.24
Page 37 and 38: 3.6 Transfer functions of the subsy
Page 39 and 40: • Converter (after linearization)
Page 41 and 42: • Fig 3.30 is current-control loo
Page 43 and 44: • The closed-loop transfer functi
Page 45: 3.9 Four-quadrant Dc motor drive•

3 Phase-controlled DC motor drives

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