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ECA1212 Introduction to Electrical & Electronics Engineering Chapter 12: Introduction to Electric Machines by Muhazam Mustapha, December 2011 Learning Outcome By the end of this chapter students are expected to: • Be able to theoretically explain the various types of electric motors • Be able to theoretically explain the various types of electric generators • Be able to mathematically solve some parameters of DC motors Chapter Content • • • • Electric Machines in General DC Machines Synchronous Machines Induction Machines Electric Machines CO1 Rotating Machines • Electromechanical machines are commonly rotational in nature • The machines require one part to be static and the other one to be rotating – Stator: stationary – Rotor: rotating • Both stator and rotor produce magnetic winding whose field will try to align each other – this produces mechanical motion CO1 Rotor and Stator Current going in Stator winding Rotor winding × × · Stator Field · Rotor Field Current coming out Stator CO1 Rotor Commutator Action Commutator reverses current in coil every half cycle There can be more than 1 pair of commutators CO1 Windings • Two types of magnetic windings: – Armature: the winding connects to load – Field: the winding only to produce field • Either armature or field winding can be located as rotor or stator • The location of field and armature determines the type of the machine CO1 Machine Types (Generator & Motor) Type DC Synchronous Induction CO1 Winding Type Location Current Type Armature Rotor DC Field Stator DC Armature Stator AC Field Rotor DC Primary Stator AC Secondary Rotor AC DC Machines CO1 DC Machines • DC Machines are hard to construct, but easiest to discuss and analyze • Hence all our mathematical discussion on machines will be on DC machines • Other machine type will be covered as theory CO1 Configurations • DC Machines can be constructed in a few configurations depending on series or parallel structure or the availability of a second power source CO1 Ra Ia Rf Lf If Vf Separately Excited La Va Configurations Lf Ra Rf Ia Vf Ra La Va Vf La Lf If Shunt Connected CO1 Series Connected Va Configurations Ra Ia Series Winding La Shunt Winding Series Winding Ia Va La Shunt Winding Short-Shunt Compound CO1 Ra Long-Shunt Compound Va Steady State Equations • Referring to the following DC machine model, we can deduce some formulas for motor and generator at constant speed CO1 Is If RS Ra Rx LS Ia VL or Vs La Rf Eb, ωm Lf Steady State Equations • Generator Eb k am T P m Eb I a m k aI a VL Eb I a Ra I S RS Ia IS I f CO1 Steady State Equations • Motor Eb k am T P m Eb I a m k aI a VL Eb I a Ra I s RS Is I f Ia CO1 Machine Constant • The armature constant of ka pN ka 2M p = number of magnetic poles N = number of conductors per coil M = number of parallel paths in armature winding CO1 Conversions 60 n m 2 n = round per minute, r/min ωm = radian per second, rad/s 1 horse power = 746 watts CO1 Synchronous Machines CO1 Alternator • Just another word for AC generator • Normally a permanent magnet or a DC powered electromagnet will be placed at rotor to generate AC current • Stator would be wound with solenoid that carries the generated energy – there can be more than one windings hence it can generate more than 1 phase of electricity CO1 Alternator × × N × · Single Phase S · · Coils at stator CO1 Three Phase Synchronous Motor • Virtually identical to alternator • Needs a DC voltage exciter at rotor to start • Called synchronous because it spins at the same rate as the AC frequency used to drive it CO1 Induction Machines CO1 Induction Motor • The stator part is almost identical to synchronous motor • AC current (single or multi-phase) will be fed into stator – produces spinning field • There is no power or permanent magnet placed in the rotor • Rotor and stator are electrically separated • Then how mechanical force is applied to the rotor? CO1 Induction Motor • Mechanical motion is possible by the induction process that is identical to the one in transformer • The changes in the magnetic flux from stator will induce current into the rotor winding and causes magnetic attraction or repel between stator and rotor poles CO1 Induction Motor • The changes of the magnetic field need to involve the cutting of the rotor coils (Faraday’s Law) • This cutting is what called ‘slip’ between the rate of stator’s field rotation and the rate of rotor’s spin • Without the slip induction machine couldn’t work CO1 Induction Motor • The ‘slippings’ also means that the rotation of rotor is not in-sync with the stator field rotation rate • This is the main electrical difference between synchronous machine and induction machine CO1 Induction Generator • Makes use of the same induction concept in induction motor – slipping process • It requires a starting power at rotor to produce magnetic field for the induction process to start • After that, the power generated by the generator itself will be used to produce the needed rotor magnetic field CO1