MEP 1523 ELECTRICAL DRIVES

16
MEP 1523 ELECTRICAL DRIVES Current ripple in unipolar and bipolar switching schemes

description

MEP 1523 ELECTRICAL DRIVES. Current ripple in unipolar and bipolar switching schemes. Current ripple. Current ripple – unavoidable in power electronic converter systems:. Undesirable because:. Zero average – increase machine heating. Ripple in torque – can be reflected in speed response. - PowerPoint PPT Presentation

Transcript of MEP 1523 ELECTRICAL DRIVES

Page 1: MEP 1523 ELECTRICAL DRIVES

MEP 1523ELECTRICAL DRIVES

Current ripple in unipolar and bipolar switching schemes

Page 2: MEP 1523 ELECTRICAL DRIVES

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

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Current ripple

H-bridge dc-dc converter with dc machine as load

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Current ripple

Approximate dc machine with RL load

H-bridge dc-dc converter with dc machine as load

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Current ripple

• Load is linear• Principle of Superposition can be applied

Vdc

Vave

Vdc

Vdc

Vave

Unipolar Bipolar

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Current ripple

Vdc

Vave

Unipolar

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Current ripple

Vdc

Vave

Unipolar

Vave

v(t) = Vave + vripple

+

i(t) = Iave + iripple

Vdc Vave

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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

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Current ripple - unipolar

iripple

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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

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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

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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

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Current ripple - bipolar

VdcVave

Bipolar

Vave

v(t) = Vave + vripple

+

i(t) = Iave + iripple

Vdc Vave

-Vdc

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Current ripple - bipolar

iripple

t

2VdcVdc-Vave

Ttri

TtridAB

triabavedc

rr TdL

VVi

ti

Lvdtdi

Lv LL

tLv

i L

i +vL

vL

iripple

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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

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Current ripple - bipolar

L2TV

i tridcmax,rr

L8TV

i tridcmax,rr

Max ripple for bipolar Max ripple for unipolar