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XIII. Finite Wave Train (Properties of the Solution) 
BquatiLons, (5623) ebhmouehya( 5c SO) eden nt on once 
XIV. Model Wave Systems with Infinitely Long Crests 
Equations i(6.1).tthnough (6.ob)P jae — tpi 
XV. An Infinite Periodic Train of Wave Groups . ‘ 
Equations (6. 7) throuchm(O.dis) ements os ot 
XVI. A Finite Train of Regular Wave Groups 
EquatHions. 6j4 iebhroneh, .(Geli7 jw ete eee) en 
XVII. Energy Considerations 
Equattonsi(6.d'6)e through ao. )eqelenuenen oy ae 
XVIII. The Lebesgue Stieltjes Power Integral 
Equations, (7.4) -throurhii( 7.10)! ot. aeaee 6 Yenee 
XIX. Some Examples 
Equatdions (7.19) through (7126) ae) iene mene 
XX. The Gaussian Case 
Equations, (7.27) ethroughaG7.34)5 ss = «6 
XXI. The Forecasting Problem for a Sea Surface 
Represented by the Gaussian Case of the Lebesgue Power 
Integral with Infinitely Long Crests in the y Direction 
Money ealosaln (HARE) venereal (eS bo 6 o 6 6 
XXII. The Forecasting Problem for a Sea Surface 
Represented by Infinitely Long Crests, a Gaussian Wave 
Record, and Winds that Lasts D_ Seconds Over a Fetch 
s 
of Length, F. 
Equations .G7,.oi.) abhrouchun@7cOl5)er ss sls lene 
XXIII. Short Crested Waves 
Equations 1 (8.2) Ghrouch s(e.>) aralse) aires 
XXIV. A Useful Lemma 
Equations, (8.6)) ,throuch GSell3) ys suis a -amenies 
XXV. The Initial Value Problem in the y,t Plane for a 
Disturbance of Finite Duration and Width 
Equations 4(8..44), throuchis(oeg7)in sneer 
XXVI. The Initial Value Problem in the y,t Plane for a 
Disturbance of Finite Duration and Width 
Equataons (esl 8)ithrenghy (G3.20)) 0. unre semeemte 
= 327,— 
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