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The mechanical effects of short-circuit currents in - Montefiore

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<strong>The</strong> first case (Figure 5.14) corresponded to the<br />

dynamic response <strong>of</strong> a system to a degree <strong>of</strong> freedom<br />

at a constant Laplace force. <strong>The</strong> second case (Figure<br />

5.15) may be resolved through a purely functional<br />

approach or by modal superposition.<br />

7.2.3.2.2.5. Reclosure<br />

When a structure has been set <strong>in</strong> motion by an <strong>in</strong>itial<br />

fault, the possibility <strong>of</strong> a recurr<strong>in</strong>g fault after<br />

reclosure may lead to <strong>in</strong>creased <strong>mechanical</strong> stresses.<br />

Between the maximum loads due to the first fault and<br />

the maximum loads result<strong>in</strong>g from the two faults,<br />

there may be a build-up factor <strong>of</strong> as much as 1.8 [Ref<br />

95]. Nevertheless, a fault recurs at reclosure roughly<br />

one out <strong>of</strong> ten times.<br />

One property, superposition, will be particularly<br />

useful <strong>in</strong> study<strong>in</strong>g reclosure.<br />

PROPERTY OF SUPERPOSITION<br />

<strong>The</strong> displacement <strong>of</strong> the system is l<strong>in</strong>ked to the<br />

excitation force by a l<strong>in</strong>ear differential operator L and<br />

denoted <strong>in</strong> the follow<strong>in</strong>g manner:<br />

r<br />

r FL<br />

( t)<br />

dur<strong>in</strong>g the <strong>short</strong> <strong>circuit</strong><br />

(5.16) L ⋅ U = r<br />

0 outside the <strong>short</strong> <strong>circuit</strong><br />

Follow<strong>in</strong>g a first fault, for a def<strong>in</strong>ite force F () t , a<br />

L<br />

fixed <strong>short</strong>-<strong>circuit</strong> <strong>in</strong>tensity, voltage phase and <strong>circuit</strong><br />

time constant, and for a given fault duration, only one<br />

physical solution describes the system's displacement<br />

over time on the basis <strong>of</strong> <strong>in</strong>itial break conditions.<br />

r r r r<br />

(5.17) U( M, 0 ) = o ∀ M<br />

r<br />

where: M : spatial variables.<br />

Follow<strong>in</strong>g a second fault, the system's response is the<br />

superposition <strong>of</strong> the dynamic responses <strong>of</strong> the faults<br />

over an <strong>in</strong>itial break condition with, however, a time<br />

lag tR correspond<strong>in</strong>g to the reclosure time:<br />

r r r r r r<br />

(5.18) U( M, t) = U1( M, t) + U2 ( M, t −tR)<br />

r r r r<br />

where U M , t)<br />

and U ( M , t)<br />

satisfy (7.16).<br />

1(<br />

2<br />

Because <strong>of</strong> this lag property, the search for the<br />

maximum follow<strong>in</strong>g the two <strong>short</strong>-<strong>circuit</strong> faults is<br />

simplified. In order to superimpose two staggered<br />

faults and calculate their optimum, all that is needed<br />

is to characterize the dynamic response <strong>of</strong> a rigid<br />

structure to each <strong>of</strong> them separately. Where the two<br />

faults are <strong>of</strong> the same type, amplitude and duration,<br />

this superposition pr<strong>in</strong>ciple is especially useful.<br />

86<br />

7.2.3.2.2.6. Comb<strong>in</strong>ed Loads<br />

Each company has to def<strong>in</strong>e its own design policy <strong>in</strong><br />

accordance with the occurrence <strong>of</strong> extreme loads. We<br />

propose here to exam<strong>in</strong>e the case <strong>of</strong> comb<strong>in</strong>ed <strong>short</strong><strong>circuit</strong><br />

and w<strong>in</strong>d loads. <strong>The</strong> action <strong>of</strong> the w<strong>in</strong>d on the<br />

busbars depends on the angle <strong>of</strong> the w<strong>in</strong>d's direction<br />

relative to the tube axis, whereas that relative to the<br />

<strong>in</strong>sulat<strong>in</strong>g bush<strong>in</strong>gs is constant for a given w<strong>in</strong>d<br />

velocity, despite its chang<strong>in</strong>g orientation. <strong>The</strong><br />

maximum dynamic response thus varies accord<strong>in</strong>g to<br />

the follow<strong>in</strong>g formula (5.19) :

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