Kremer E.'s A (New) burning cost method in case of trend PDF

By Kremer E.

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1. '«.. 2ZUZZ2Z22 --- ---- -- - --- ------------- --- -- ·· .. ,. -. -.. -\ -,. -1-1- l' ··· ... f. -. ,. ~. ,_,_ ,. • '. -,-'. ,. ,. ,. -. -~,. , .. -t-- ,. ,-.. Zltzl lUln? x x [[]J1] 3 . ·. ... ··. , -I-,------- - -,. ----. -:-:- ':"_--_;) -t-,-' ... ,_ ' ,-------, ~ ·• . ·. ~ o • • Ie ZZ2222222122IZZ , ... , ~ lZZlztzt?? 2 - - .... :- 0:.. --. ): . -a- , - l U l l . l1111 _I _I. 3 :(: 25 :):G c:) ~:. x x I . - ,:" __ ,, 1 \ -, - I ... 3 Figo 19o Field patterns of rectangular-waveguide modes.

F. -. ,. ~. ,_,_ ,. • '. -,-'. ,. ,. ,. -. -~,. , .. -t-- ,. ,-.. Zltzl lUln? x x [[]J1] 3 . ·. ... ··. , -I-,------- - -,. ----. -:-:- ':"_--_;) -t-,-' ... ,_ ' ,-------, ~ ·• . ·. ~ o • • Ie ZZ2222222122IZZ , ... , ~ lZZlztzt?? 2 - - .... :- 0:.. --. ): . -a- , - l U l l . l1111 _I _I. 3 :(: 25 :):G c:) ~:. x x I . - ,:" __ ,, 1 \ -, - I ... 3 Figo 19o Field patterns of rectangular-waveguide modes. 318 x 1O-4yE,:""ab ( -mb -+ mb na 2 ;i 1- (A)2 Ac (41) where Eb is the maximum electric field intensity, which occurs at values of x and y such that \.

I985 Howard W. Sams &: Company; reproduced with permission) The dielectric loss in a microstrip line in nepers per meter is [6] ad Jr Jr [ ~( = Ag (tand)eff = Ag tand 1 + t 1FF +- 1)] 1 Er where F = VI + lOhlW and the guide wavelength Ag is calculated from (19b). \ \ >, '-~,. \ \ (20) Related Topics 28-32 The conductor loss in nepers per meter due to the dissipation in the strip and ground plane is (21) where ZI is the characteristic impedance of the corresponding air-filled lossless microstrip line obtained by (19), and Zt'J is calculated with the same formula by replacing W, h, and t with W', h', and t ' such that W'=W_(} h' = h + (} t' = t - (22) (} where (} (= V2/wJloa) is the skin depth.

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A (New) burning cost method in case of trend by Kremer E.


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