Linearized Potential Flow Theory for ACVs in a Seaway 



wave potential $0001 an ^ the hydrostatic pressure will, of course, 

 be the same on both sides. The hull functions h 1 and h 2 have 

 therefore been combined in these cases to give the total width h . 

 In the case of the potentials involving the cushion pressure namely, 

 ^0100 and ^0101 , the two sides are considered separately. 



The final result is 



H 



// 



- Zb o v *iooo (x '' b ' z,) a 



ah 



i, 



( ^ h l d h 2 



f X 1 X 1 



2 6 a e p 



V< x 



ah 



+ z. 



ah 



ooi ax' ooi az' 



/-; r~ ^h , dh ) 



+ ^ooi (z +h G"ax-- " x T7- > *1000 



/ x'x' 



+ (v *ioio , - i(r<I> ioio) a 



ah 



■?s/Q i<Tt 

 - 2 5 Pa e p 



V/x 



001 ax' Z 001 dz ! 



a h i 



+ %oi (z, + h c a x 



- x . 4^ l + 



az- roioo 



+ (V# - icr$ ) --.-^- + 



v oiio . ono ; a x * 



S h 2 



3 h ; 



+ Vx ooi "5?" + z ooi "5 



d h 2 



+ (z'+h 



oor g ^x 



h\ 



$ 



0100 



+ (v *ono , --♦oiio) 1^1 ' 



x' 



197 



