Mikrovalna elektronika - FESB

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MIKROVALNA ELEKTRONIKA <strong>FESB</strong> – SPLIT U ovoj jednadžbi sada pretpostavljamo da je amplituda izmjeničnog napona u R1 mnogo manja od katodnog napona, i izraz u zagradi razvijamo u binomni red te zadržimo prva dva člana reda, pri čemu članove višeg reda zanemarujemo, pa je: gdje je: V V V 1 ωt ωt θ ⎛ ⎞
MIKROVALNA ELEKTRONIKA <strong>FESB</strong> – SPLIT 3 2 M = 1,84 M = 1,0 M = 0,5 faza prolaza R1 (rad) 1 0 -1 -2 -3 -1.5 -1 -0.5 0 0.5 1 1.5 faza dolaska na R2 (rad) Slika 3. Ovisnost faze prolaza kroz R1 o fazi dolaska na R2 6 5 M = 0,5 M = 1 M = 1.84 4 G2/G0 3 2 1 0 -1.5 -1 -0.5 0 0.5 1 1.5 faza dolaska na R2 (rad) Slika 4. Ovisnost struje klistrona o fazi dolaska na R2 za različite vrijednosti M - 161 -
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MIKROVALNA ELEKTRONIKA FESB - SPLIT
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odnosno: rot Etr = − jωµ ezH
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Izračunajmo sada snagu prenesenu n
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Page 109 and 110: MIKROVALNA ELEKTRONIKA FESB - SPLIT
Page 125 and 126: d N = r × F , dt MIKROVALNA ELEK
Page 129 and 130: odnosno: uz: iz čega je: pa je:
Page 157 and 158: V 0 Slika 1. Dvorezonantni klistron
Page 159: MIKROVALNA ELEKTRONIKA FESB - SPLIT
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Mikrovalna elektronika - FESB

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