dc machine
DESCRIPTION
elecTRANSCRIPT
7/21/2019 DC Machine
http://slidepdf.com/reader/full/dc-machine-56da066a6c563 1/3
D.C. MACHINES .Working principle of D.C.Machine as generator and motor, constructional
features, EMF equation of generator and simple problems, back emf and torque
equation of DC motors, simple problems, types of DC motors, characteristics and
applications, necessity of starter, 3point starter.
______________________________________________________________________ A machine which works on direct current is defined as a D.C.Machine.
D.C.Machines are of two types. !i" D.C.#enerator and !ii" D.C.Motor.
Sl.No. D.C. #enerator D.C.Motor
Definition$
A !enerator is a rotatin!
machine which con"ertsmechanical ener!y into
electrical ener!y
Definition$
A motor is a machine which
con"erts electrical ener!y intomechanical ener!y
# %rinciple$$hene"er a coil is rotated
in a ma!netic field ane.m.f. will %e induced in
this coil
and is !i"en %y
e&'l"Sin( "olts)coil sidewhere* '&+he flu, density
in +esla* l&the acti"e len!th
of the coil side in meters*"&the "elocity with which
the coil is mo"ed inmeters)sec and ( is thean!le %etween the direction
of the flu, and the
direction of rotation of the
coil side.
%rinciple$$hene"er a current coil is
placed under a ma!netic fieldthe coil e,periences a
mechanical force* and is !i"en
%y -& 'IlSin( Newtons)coil
side.$here* I is the current throu!h
the coil in ampere.
+he direction of the emf
induced is fi,ed %yapplyin! the -lemin!/s
ri!ht hand rule
+he direction of the force
actin! is fi,ed %y applyin! the-lemin!/s left hand rule.
C&'()*+C)&' &F - D.C.M-C'E.
Salient parts of a D.C.machine are0
• -ield system 1poles2
• Coil arran!ement 1armature2
• Commutator
• 'rushes
7/21/2019 DC Machine
http://slidepdf.com/reader/full/dc-machine-56da066a6c563 2/3
• 3oke
-i! shows the details of a four pole D.C. machine with %oth shunt and series fieldwindin!s.
Field system0 +his is made of electroma!nets* wherein a iron laminated core is
wound with well insulated enameled copper wire. +he core is laminated tominimi4e the eddy current loss. Each lamination is dipped in "arnish and dried. A
pole shoe is attached to the pole face to direct the flu, to concentrate radially on to
the armature there%y reducin! the leaka!e and frin!in! flu,. 5oles are fi,ed to theyoke %y means of %olts.
-rmature0 +his is the rotatin! part of the machine made of laminated iron core
cylindrical in structure with slots on its periphery. Insulated copper coils are laid in
these slots* and these coils are connected for lap or wa"e connection. +he corelaminations are firmly mounted on a shaft fitted with smooth %earin!s on either side
for smooth rotation.
Comparison of lap and /a0e /indings01-% W-2E
Num%er of armature parallel paths
is e6ual to the num%er of poles.
Num%er of parallel paths is always
e6ual to two.
5referred when lar!e current at
lesser "olta!e is the re6uirement.
5referred when lar!e "olta!e with
lesser current is the re6uirement.
Commutator$ As the induced e.m.f. in the armature is alternatin! commutator
con"erts alternatin! e.m.f. into unidirectional e.m.f.+his is cylindrical in structure made of copper se!ments with mica insulation
%etween them and is firmly fi,ed on to the shaft carryin! the armature and the
armature coil free ends are %ra4ed to the commutator se!ments.rushes$ +hese are current collectin! de"ices placed on the %ody of the
commutator with a holder. 'rushes are made of car%on* copper or !raphite.
4oke$ +his is the outer most part of the machine made of cast steel which is the
mechanical enclosure for the machine to protect it from dust and moisture and also pro"ides the return path for the ma!netic flu, and carries half the flu, per pole.
E.M.F. Equation$
7et the D.C. machine has % num%er of poles* 5 num%er of armature conductors
arran!ed in - num%er of parallel paths. 7et 6 %e the flu, per pole and ' is the
speed of rotation in re"olutions per minute.
Consider one North 5ole of the machine under which a !roup of armatureconductors all %ein! connected in series. 7et 7 %e the spacin! %etween any two
nei!h%orin! conductors ant t %e the time taken to mo"e throu!h this distance of 7.
+he total flu, per pole 6 is made of se"eral lines and one line of flu, is cut %y oneconductor when it mo"es throu!h a distance of 7 in t seconds.
+herefore the induced emf in the st conductor when cut %y the flu, of 68
ise & 689t "olts
7/21/2019 DC Machine
http://slidepdf.com/reader/full/dc-machine-56da066a6c563 3/3
Similarly in the #nd conductor e# & 6:9t "olts* and so on.
+herefore the total emf induced in all the conductors under one pole is the sum ofall these emf/s.
E& e 8 e# 8 e 8 e9 8 ::..E& 689t ; 6:9t ; 639t ; 6<9t ; ==..
E& 69t "olts)pole. -or all the 5 num%er of poles E& %69t "olts+he speed is defined as ' re"olutions per minute*
' re"olutions in one minute or >? seconds.
re"olutions will %e in time of >?9' seconds* and as one re"olution corresponds to
all the 5 num%er of conductors the time t for a tra"el of distance 7 can %e written as
t@ >?9'5 seconds.
+herefore the induced EM- E@ %69t @ %69>?9!'5"@%5'69>?.
As the ; num%er of conductors are arran!ed in A num%er of parallel paths*
+he induced e.m.f per parallel path is
E@ %5'69>?- "olts.
As %, 5, - are fi,ed the induced e.m.f is mainly dependent on the flu, and the
speed* and hence we write that the induced e.m.f E is proportional to the product of
the speed ' and the flu, 6.