WAVE 
RESISTANCE 
(Continued) 
T. H. HAVELOCK 
with ship) resulltse seme roc ene 
more complicated pressure systems... 
moving surface pressure system, start- 
ING} MOMBLEStink! cela ceimiels «ene ela we ls 
circular cylinder, starting from rest... 
Ti SRSEGNY THOM 5 os 00 ad0b0 000000000 
of a submerged body equal to that of a 
certain travelling pressure distribution 
SP ere yoAiecienca setter habs cathe motores 
GIO Uh, SAFES o600000000000000600608 
in parallel we ee eee he he ele 
in any relative position...........5. 
general elltpsoid..............-.+-- 
vertical posts, of great draught, vary- 
ing waterplane sections............. 
with insertion of parallel body....... 
of finite draught, effect of varying 
GrAUP Gar wearers cue vereeccmete arcue ere eevee 
of great draught comparison of a sym- 
metrical with an unsymmetrical 
Waterline hiatieiis: oi saris slewercresre,« 
parabolic waterplane ............... 
derived from wave patterns .......... 
derived by energy method from wave 
pattern deep and shallow water ...... 
of unsymmetrical forms used to esti- 
mate wave resistance in a viscous 
PLUG eg eeeroeye atte aeerccaneaseine ooo oeats 
Mutual action of two bodies ......... 
GORCHEL GGORY c006 00000000040 000005 
CWO) 'SpRene|s AMVSCLICSh ess). sacl) eee 
in parallel, (alsoone sphere near wall) 
in any relative position............. 
approximate calculation at high speed 
comparison with complete calculation 
and with experimental results for a 
form with an algebraic equation...... 
Comparison with experiments for two 
IMOGIENS OF SININSsc5coovccoooapccoode 
Effect of shallow water............. 
230 
245,256 
388 
385-389 
390-397 
398-407 
408-418 
403 
413 
415 
417 
500-511 
511 
511 
192 
51-57 
