n' -^n 



h* 



CD 



CDl 



Cd2 = CD2 



CdPi = CDPl 

 C^„ - CDVl 



Cdp. ^ CDP2 



Cdv^ = CDV2 



Bl^^ = B1(K,J) 

 B2j = B2(K,J) 

 DlJ = D1(K,J) 

 D2j = D2(K,J) 



Y. - Y(J), Ylj - Y1(J) 



Y2j - Y2(J) 



PRETl 



PREPl 



T..; 1-1. PRECl 



PRESl 



PRET2 y 

 PREP 2 

 PREC2 

 PRES2 



PRESS 



PRESI 



ERl, ER21, ER22 



Desai and Lieber 



Refer to definition in Eq. (2.50) 



The physically infinite distance for the iterative 

 solutions 



Total drag coefficient 



Total first iteration drag coefficient 



Total second iteration drag coefficient 



First iteration pressure drag coefficient 



First iteration viscous drag coefficient 



Second iteration pressure drag coefficient 



Second iteration viscous drag coefficient 



Space variables defined by r = e*^^ = e^^"^ '^ "^) 



Constants in the power series expansion of B^ 



Constants in the power series expansion of -Ji^ 



Constants in the power series expansion of D^ 



Constants in the power series expansion of D^ 



Kronecker delta 



Constants involved in the first iteration solution 



Constants involved in the second iteration solution 



Fourier components of the pressure fields pj and p^ 

 as defined in Part 3 of this paper 



Potential flow pressure field 



Measures of error due to the assumptions 



VO = 0, D^(r) - 0, n > 3 



492 



