MEP 1523 ELECTRICAL DRIVES
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MEP 1523ELECTRICAL DRIVES
Current ripple in unipolar and bipolar switching schemes
Current ripple – unavoidable in power electronic converter systems:
Current ripple
Undesirable because:
• Zero average – increase machine heating
• Ripple in torque – can be reflected in speed response
• Ratings of devices must consider ripple - higher rating of peak current
Current ripple
H-bridge dc-dc converter with dc machine as load
Current ripple
Approximate dc machine with RL load
H-bridge dc-dc converter with dc machine as load
Current ripple
• Load is linear• Principle of Superposition can be applied
Vdc
Vave
Vdc
Vdc
Vave
Unipolar Bipolar
Current ripple
Vdc
Vave
Unipolar
Current ripple
Vdc
Vave
Unipolar
Vave
v(t) = Vave + vripple
+
i(t) = Iave + iripple
Vdc Vave
Current ripple - unipolar
i(t) = Iave + iripple
= +
i(t) Iave iripple
Switching frequency is high
- Impedance of AC component dominated by L
- Ripple is calculated based on v-i relation of L
- L appear as short circuit in DC
Current ripple - unipolar
iripple
Current ripple - unipolar
iripple
t
VdcVdc-Vave
Ttri
T
TdAB
TdL
VVi ab
avedcrr
ti
Lvdtdi
Lv LL
tLv
i L
i +vL
vL
iripple
Current ripple - unipolar
TdL
VVi ab
avedcrr
but Vave = dabVdc
TVL
ddi dc
2abab
rr
, maximum when dab= 0.5
tridc
2
max,rr TVL2
5.05.0i
L8TV
i tridcmax,rr
It can be shown that for bipolar scheme,
L2TV
i tridcmax,rr
Max current ripple in bipolar scheme is four times that of unipolar scheme
Current ripple - bipolar
VdcVave
Bipolar
Vave
v(t) = Vave + vripple
+
i(t) = Iave + iripple
Vdc Vave
-Vdc
Current ripple - bipolar
iripple
t
2VdcVdc-Vave
Ttri
TtridAB
triabavedc
rr TdL
VVi
ti
Lvdtdi
Lv LL
tLv
i L
i +vL
vL
iripple
Current ripple - bipolar
triabavedc
rr TdL
VVi
but Vave = (2dab1)Vdc
tridc
2abab
rr TV2L
ddi
, maximum when dab= 0.5
tridc
2
max,rr TV2L
5.05.0i
L2TV
i tridcmax,rr
Current ripple - bipolar
L2TV
i tridcmax,rr
L8TV
i tridcmax,rr
Max ripple for bipolar Max ripple for unipolar