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Ma{instvo 2(7), 63 – 74, (2003)<br />

N.[virig;....: ANALIZA NAPREZANJA U U^VR[^ENJU...<br />

Slika 5.9. Raspored <strong>naprezanja</strong> i reda izokroma po konturi, za model VI<br />

Figure 5.9. Stress arrangement and isochrome order along the contour for model VI<br />

6. ZAKLJU^AK<br />

Raspodjela <strong>naprezanja</strong> na kriti~nim mjestima<br />

u~vr{}enja pola <strong>generatora</strong>, bilo u obliku lastinog<br />

repa, ~eki}a ili pak njihove kombinacije, takova je<br />

iznosa da ih treba uzeti u obzir kod mehani~kih<br />

prora~una tih elemenata.<br />

Najve}i faktor koncentracije <strong>naprezanja</strong> javlja se pri<br />

modelima kod kojih je korijen pola izra|en u<br />

obliku lastinog repa ( model V ), budu}i je kod<br />

tog oblika najizra`eniji utjecaj radijusa zakrivljenosti<br />

na prijelazu tijela pola u korijen pola (sl. 5.8.).<br />

Na modelu I a posebno na modelima II – IV, faktor<br />

koncentracije <strong>naprezanja</strong> je upola manji u odnosu na<br />

model V (tablica 5.3.) {to je s jedne strane<br />

posljedica smanjenog utjecaja zareznog djelovanja<br />

(bla`i je prijelaz s tijela pola na njihov korijen), a s<br />

druge strane dosjedne povr{ine izme|u korijena pola<br />

i utora u lan~anom prstenu se pove~avaju s<br />

porastom kuta γ.<br />

Kod korijena <strong>polova</strong> u obliku ~eki}a i kombinacije<br />

~eki}-lastin rep dio <strong>naprezanja</strong> prenosio se du`<br />

vrata ~eki}a te se ukupno optere}enje ne<br />

koncentrira samo na presjek I-I (sl. 5.5.) kao pri<br />

modelu V, {to tako|er utje~e na znatno smanjenje<br />

koncentracije <strong>naprezanja</strong> na kriti~nim presjecima.<br />

Treba jo{ napomenuti da bi se dodatnim<br />

ispitivanjima trebao definirati optimalni kut nagiba γ.<br />

6. CONCLUSION<br />

Stress arrangement in critical points of the generator<br />

pole fixing, regardless of the type of fixing, i.e.<br />

swallow’s tail, hammer or their combination, are such<br />

that their values should be taken into consideration<br />

when the strength of these elements is calculated.<br />

The biggest stress concentration factor occurs with<br />

models whose pole root has the shape of the<br />

swallow’s tail (model V), since this shape shows<br />

the influence of radius roundness on the spot<br />

where pole body becomes pole root.<br />

On model I and particularly on models II – IV, stress<br />

concentration factor decreases considerably (Table<br />

5.3.) due to smaller influence of radius roundness<br />

(the transition from the body to the root is more<br />

temperate), whereas, on the other hand, the contact<br />

surface between the pole root and the groove in the<br />

chain ring increase as the angle γ increase.<br />

With pole roots in the shape of a hammer and the<br />

combination hammer-swallow’s tail, a portion of the<br />

stress is transmitted along the hammer neck and<br />

consequently, the total load is not concentrated on the<br />

cross section I – I only, (Fig. 5.5) as is the case with<br />

the model V. This also influences the stress<br />

concentration causing it to decrease at critical cross<br />

sections. It is also worth mentioning that additional<br />

tests should define optimal angle of the slope, γ.<br />

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