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Category:

Thesis, nostrification

Type:

praca doktorska pracowników zatrudnionych w PG oraz studentów studium doktoranckiego

Language:

Polish

Publication year:

2017

Bibliography: test

1. Rys. 3.11. Wyniki symulacji MEB dla różnych wartości δμ. Wykresy przedstawiają kolejno rozkłady przestrzenne: (a) B x (x), (b) B z (x) oraz c) ∂B z (x)/∂x. open in new tab
2. Rys. 3.15. Wyniki symulacji MEB dla różnych wartości zmiany szerokości próbki δw. Wykresy przedstawiają kolejno rozkłady przestrzenne: (a) B x (x), (b) B z (x) oraz (c) ∂B z (x)/∂x. open in new tab
3. Analogiczne podejście jak w przypadku prezentacji wyników widocznych na open in new tab
4. Rys. 4.18 i Rys. 4.19 zastosowano do przedstawienia rezultatów symulacji otrzymanych dla składowej indukcji B z . Zgodnie z powyższym na Rys. 4.20 również umieszczono zestawienie rozkładów przestrzennych składowej indukcji B z przy dwóch różnych prędkościach: 0,01 open in new tab
5. Rys. 4.20, są zauważalne gołym okiem. Jak widać rozkład przestrzenny składowej indukcji B z open in new tab
6. Rys. 4.18. Porównanie przestrzennych rozkładów składowej indukcji B x pomiędzy biegunami open in new tab
7. m/s przedstawiono na Rys. 4.21. Można stwierdzić, iż zakres wartości dla zmiany δB z Rys. 4.20. Porównanie przestrzennych rozkładów składowej indukcji B z pomiędzy biegunami magneśnicy, uzyskanych dla prędkości 0,01 i 1 m/s open in new tab
8. Rys. 4.19. Zależność przestrzenna zmiany δB x wartości składowej indukcji B x , która zachodzi przy wzroście prędkości od 0,01 do 1 m/s open in new tab
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