DC Machine A Presentation on Submitted to : Department of Electrical Engg. Atmiya Institute of Tech. & Sci. Rajkot (003)

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Presentation transcript:

DC Machine A Presentation on Submitted to : Department of Electrical Engg. Atmiya Institute of Tech. & Sci. Rajkot (003)

Contents – Overview of Direct Current Machines – Construction – Principle of Operation – Types of DC Motor – Power Flow Diagram

DC motor principles DC motors consist of rotor-mounted windings (armature) and stationary windings (field poles). In all DC motors, except permanent magnet motors, current must be conducted to the armature windings by passing current through carbon brushes that slide over a set of copper surfaces called a commutator, which is mounted on the rotor. Parts of an electric motor The commutator bars are soldered to armature coils. The brush/commutator combination makes a sliding switch that energizes particular portions of the armature, based on the position of the rotor. This process creates north and south magnetic poles on the rotor that are attracted to or repelled by north and south poles on the stator, which are formed by passing direct current through the field windings. It's this magnetic attraction and repulsion that causes the rotor to rotate.

The Advantages The greatest advantage of DC motors may be speed control. Since speed is directly proportional to armature voltage and inversely proportional to the magnetic flux produced by the poles, adjusting the armature voltage and/or the field current will change the rotor speed. Today, adjustable frequency drives can provide precise speed control for AC motors, but they do so at the expense of power quality, as the solid-state switching devices in the drives produce a rich harmonic spectrum. The DC motor has no adverse effects on power quality.

The drawbacks Power supply, initial cost, and maintenance requirements are the negatives associated with DC motors Rectification must be provided for any DC motors supplied from the grid. It can also cause power quality problems. The construction of a DC motor is considerably more complicated and expensive than that of an AC motor, primarily due to the commutator, brushes, and armature windings. An induction motor requires no commutator or brushes, and most use cast squirrel-cage rotor bars instead of true windings — two huge simplifications.

Major types of dc motors Self excited dc motor – Series dc motor – Shunt dc motor – Compound dc motor Separately excited dc motor Permanent magnet dc motor

Series motors Series motors connect the field windings in series with the armature. Series motors lack good speed regulation, but are well-suited for high- torque loads like power tools and automobile starters because of their high torque production and compact size. EaEaEaEa RfRfRfRfM V T (dc supply) RaRaRaRa iaiaiaia

Series Motor Power Flow Diagram PPPP P out P in = V T i L P ca =i a 2 R a P cf =i a 2 R f PmPm P  is normally given P in = P out + total losses Where, P ca =armature copper loss P cf =field copper loss P  =stray, mech etc P m = E a i a

Shunt motors Shunt motors use high- resistance field windings connected in parallel with the armature. Varying the field resistance changes the motor speed. Shunt motors are prone to armature reaction, a distortion and weakening of the flux generated by the poles that results in commutation problems evidenced by sparking at the brushes. Installing additional poles, called interpoles, on the stator between the main poles wired in series with the armature reduces armature reaction. EaEa V T (dc supply) RaRa iaia ifif RfRf M iLiL

Shunt Motor (power flow diagram) PPPP P out P in =V T i L P ca =i a 2 R a P cf =i f 2 R f PmPm P  is normally given P in = P out + total losses Where, P ca =armature copper loss P cf =field copper loss P  =stray, mech etc P m = E a i a

Compound motors the concept of the series and shunt designs are combined. EaEa V T (dc supply) RaRa iaia ifif R f1 M iLiL R f2

Compound motor (power flow diagram) P  is normally given P in = P out + total losses Where, P ca =armature copper loss P cf =field copper loss P  =stray, mech etc P m = E a i a PPPP P out P in =V T i L P ca =i a 2 R a P cf1 =i f 2 R f1 PmPm P cf2 =i a 2 R f2

Separately Excited Motor There is no direct connection between the armature and field winding resistance DC field current is supplied by an independent source – (such as battery or another generator or prime mover called an exciter)

Separately Excited Motor (Cont) Where p= no of pole pair n= speed (rpm) Z=no of conductor  =Flux per pole (Wb) C= no of current/parallel path =2p (lap winding) =2 (wave winding) KVL: Circuit analysis: EaEa RaRa LaLa iaia M RfRf VTVT VfVf LfLf IfIf