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Transformer models in EMTP/ATP

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Core representation<br />

• Attached to the fictitious N+1th w<strong>in</strong>d<strong>in</strong>g<br />

• Topologically “correct” core model, with<br />

nonl<strong>in</strong>ear <strong>in</strong>ductances represent<strong>in</strong>g<br />

each leg and limb<br />

– Triplex<br />

– 3- and 5-legged core<br />

• Flux l<strong>in</strong>kage-current relation by Frolich<br />

equation and relative lengths and<br />

areas.<br />

• Fitt<strong>in</strong>g to Test Report<br />

λ<br />

i<br />

λ =<br />

a'<br />

+ b'<br />

⋅|<br />

i |<br />

i<br />

R o<br />

L l R l<br />

L o<br />

R y<br />

L y<br />

L l R l<br />

R y<br />

L y<br />

L l R l<br />

R o<br />

L o<br />

15 / 19<br />

11/6/2012<br />

<strong>Transformer</strong> model<strong>in</strong>g at high<br />

frequency<br />

• <strong>Transformer</strong> <strong>models</strong> <strong>in</strong> <strong>EMTP</strong> are valid for<br />

frequencies up to 2 kHz<br />

• To study phenomena with characteristic frequency <strong>in</strong><br />

range of 2 - 30 kHz, capacitive coupl<strong>in</strong>g among<br />

w<strong>in</strong>d<strong>in</strong>gs and to ground must be added<br />

• Above 30 kHz a more detailed representation of<br />

<strong>in</strong>ternal w<strong>in</strong>d<strong>in</strong>g arrangement is required<br />

– Interw<strong>in</strong>d<strong>in</strong>g and <strong>in</strong>terturn/disks capacitances must be taken<br />

<strong>in</strong>to account<br />

• Above 100 kHz the presence of ferromagnetic<br />

material has just secondary importance.

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