Dc motor
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Transcript of Dc motor
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03/07/151
Welcome to
Lectures on D.C.Machine
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D. C. Generator
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Portable D. C. Generator
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DIRECT CURRENT MACHINES
DC machine Construction
• The major advantages of DC machines are: easy speed and torque regulation.
• The stator of the DC motor has poles, which are excited by DC current to produce magnetic fields.
• The rotor has a ring-shaped laminated iron-core with slots.
• Coils with several turns are placed in the slots. The distance between the two legs of the coil is about 180 electric degrees.
N S
Stator with with polesBrush
Rotor
Field
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D. C. Generator
Principle of Operation
When a conductor rotates in a magnetic field, dynamically induced e.m.f is produced in it according to Faraday’s law of electromagnetic induction
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Generated EMF
Let
Ei.epathsparalleltheofoneanyingeneratedEMFEEMFGenerated
ArmatureinpathparallelanyininducedEMFE
rpminrotationArmatureN
ArmatureinPathsParallelofNo.A
polesGeneratorofNo.P
SlotperConductorsofNo.SlotsofNo.
ConductorsArmatureofNo.TotalZ
WbinFlux/Poleφ
g =
====
×===
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secN
60dt,revolution1forTime
N/60s/secRevolutionofNo.
WbφPdφ,revolution1intorcut/conducFluxNow,
voltdt
dφConductorGenerated/EMFAverage
=∴
==
=
Hence, according to Faraday’s Laws of electromagnetic induction,
volt60
φPN
60/N
φP
voltdt
dφconductorGenerated/EMF
==
=
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For Wave wound Generator
No. of Parallel Paths = 2
No. of Conductors (in series) in 1 path = Z/2
volt120
φZPNvolt
260
φPNpathGenerated/EMF =×= Z
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For Lap wound Generator
No. of Parallel Paths = P
No. of Conductors (in series) in 1 path = Z/P
volt60
φZNvolt
P60
φPNpathGenerated/EMF =×= Z
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In General,
Generated EMF
windinglapforP
windingwavefor2Awhere,
voltA
P
60
φZNE g
==
=
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Also,
voltA
P
π
ωφZvolt
A
PφZ
πN
πEg
=
=
260
2
2
1
For a given D.C. Machine, Z, P and A are constants
Hence, Putting
rps)inis(N
voltsφNk2π
ωφkE
get,we,A
ZPk
aag
a
==
=
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Types of D.C. Generators
According to the way in which their fields are excited, generators are classified into :
i) Separately excited D.C. Generatorii) Self- excited D.C. Generator
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i) Separately excited D.C. Generators are those whose field magnets are energized from an independent source of D.C. Current
DropsBrushIREV ag −−=Ra = Armature Resistance
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ii) Self excited D.C. Generators are those whose field magnets are energized by the currents produced by the generators themselves.
There are 3 types of self-excited D.C. Generators named according tothe manner in which their field coils are connected to the armature.
These are :
• Shunt wound D.C. Generator• Series wound D.C. Generator• Compound wound D.C. Generator
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i) Shunt wound D.C. Generator
Rsh – Shunt Field ResistanceRa - Armature Resistance
sha III +=
DropsBrushRIEV aag −−=
shsh RIV =
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ii) Series wound D.C. Generator
DropsBrush)RR (IEV seaag −+−=
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iii) Compound wound D.C. Generator
Short Shunt
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Long Shunt
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Ex.1 A D.C. Shunt Generator delivers 450A at 230V and the resistance of the shunt field and armature are 50Ω and 0.03 Ωrespectively. Calculate the generated EMF.
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Ex.2 An 8 - pole D.C. Shunt Generator with 778 wave wound armature conductors running at 500 rpm suppliesa load of 12.5Ω resistance at terminal voltage of 250V.The armature resistance is 0.24Ω and the field resistance is 250Ω .Find the armature current, the generated EMF and the flux per pole.