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The mechanical effects of short-circuit currents in - Montefiore

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the electromagnetic force at 2f is two times higher and<br />

the constant term is zero. For fc/f < 1 outside the<br />

resonances, the stress for the outer phases L1, L3 is<br />

higher caused by the constant term.<br />

<strong>The</strong> amplifications due to resonance require that the<br />

stress <strong>in</strong> the conductor is always <strong>in</strong> the elastic range. In<br />

fact, dur<strong>in</strong>g or near resonance the stress will <strong>in</strong>crease as<br />

far as plasticity is reached. By this the <strong>mechanical</strong><br />

frequency <strong>of</strong> the conductor is shifted to lower values<br />

and the condition for resonance which is only valid <strong>in</strong><br />

the elastic range is no longer met. Because the <strong>in</strong>crease<br />

<strong>of</strong> the stress due to resonance needs a constant<br />

eigenfrequency resonance, resonance phenomena<br />

cannot occur <strong>in</strong> plastic limit state [Ref 23]. <strong>The</strong> factor<br />

Vσ cannot become greater than 1. <strong>The</strong> dynamic<br />

calculation is equivalent to a static calculation with the<br />

maximum values <strong>of</strong> the electromagnetic force as a static<br />

equivalent force which cause the ultimate load MTr<br />

accord<strong>in</strong>g to equation (2.27). Lower outer moments give<br />

elastic or elastic-plastic deformations lower than the<br />

ultimate load, but equations (2.28) and (2.29) are always<br />

fulfilled.<br />

Figure 2.2 is calculated for beams fixed at both ends. In<br />

substations, the conductors are mounted on <strong>in</strong>sulators<br />

which are elastic and can oscillate. Thus there are no<br />

fixed supports. For fc > f, the amplifications by<br />

resonance are clearly reduced and also the range <strong>in</strong><br />

between [Ref 20, Ref 24]. For the simplified method it<br />

is sufficient to state a curve which lies near the m<strong>in</strong>ima<br />

<strong>in</strong> Figure 2.2. Attention should be payed to the fact, that<br />

the calculated curves are related to the maximum force<br />

at L1, L3 and the standardised one is related to the<br />

maximum force at L2, which differ by about 7 %.<br />

If the verification for the <strong>short</strong>-<strong>circuit</strong> strength is done<br />

without consideration <strong>of</strong> the conductor frequency, a<br />

calculation with the maximum Vσ = 1 can be done, this<br />

value is stated <strong>in</strong> Table 2 <strong>of</strong> the standard. <strong>The</strong> use <strong>of</strong><br />

values Vσ < 1 especially with HV-arrangements needs<br />

the knowledge <strong>of</strong> the conductor frequency, which is<br />

shown <strong>in</strong> sub-section 2.2.4.<br />

16

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