The mechanical effects of short-circuit currents in - Montefiore
The mechanical effects of short-circuit currents in - Montefiore
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) :