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762 BASIC CONTROL SYSTEMS


Only thecontinuous conductionmode of operation of the drive for motoring and regenerative
braking will be considered here. The angleαcan be greater or less thanγ, which is the angle at
which the source voltagevsis equal to the back emfE,

γ=sin−^1

(
E
Vm

)
(16.1.21)

whereVmis the peak value of the supply voltage. For the case ofα<γ, waveforms are shown in
Figure 16.1.13(a) for the motoring operation. It is possible to turn on thyristorsT 1 andT 3 because
ia>0, even thoughvs<E. The same is true for thyristorsT 2 andT 4.
WhenT 1 andT 3 conduct during the intervalα≤ωt≤(π+α), the following volt–ampere
equation holds:

vs=E+iaRa+La

dia
dt

(16.1.22)

Multiplying both sides byiat, wheretis a small time interval, we obtain

vsiat=Eiat+i^2 aRat+Laia

(
dia
dt

)
t (16.1.23)

in which the terms can be identified as the energy supplied or consumed by the respective elements.
Figure 16.1.13(b) corresponds to the regenerative braking operation, in which

γ′=π−γ=π−sin−^1

(
|E|
Vm

)
(16.1.24)

andαcan be greater or less thanγ′.
WhenT 1 andT 3 conduct, Equation (16.1.22) describes the motor operation withE=Kmωm.
Thus,

va=La

dia
dt

+Raia+Kmωm=Vmsinωt (16.1.25)

Similarly, whenT 2 andT 4 conduct,

va=La

dia
dt

+Raia+Kmωm=−Vmsinωt (16.1.26)

whereωis the supply frequency,ωmis the motor speed, andKmis the motor back emf constant.

(a)

ωt

va

T 1 , T 3 T 2 , T 4

E

va

ia ia
ia

−vs vs

(^0) αγ ππ + α 2 π
(b)
ωt
vs
T 2 , T 4 T 1 , T 3 T 2 , T 4
E
−vs
ia
va va
(^02) π
γ′ γ
α π
Figure 16.1.13Continuous conduction mode of operation.(a)Motoring (case shown forα<γ).(b)re-
generative braking (case shown forα<γ′).

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