• Nie Znaleziono Wyników

On the calculation methods of wave induced vibration of ships.

N/A
N/A
Protected

Academic year: 2021

Share "On the calculation methods of wave induced vibration of ships."

Copied!
14
0
0

Pełen tekst

(1)

^ Technische Hogeschool

DeKt

g ^ l ^ C T ) Wave Induced Vibration % \ % ^ \ t

ffl ^ 3t

mm

m 4 0

su

m

BH ?n 48 11

(2)

On t h e C a l c u l a t i o n M e t h o d s o f Wave I n d u c e d

V i b r a t i o n o f S h i p s

By F u k u z o T A S A I

I n t h i s p a p e r we h a v e d i s c u s s e d a b o u t t h e

c a l c u l a t i o n m e t h o d o f w a v e i n d u c e d v i b r a t i o n o f

a s h i p a d v a n c i n g i n w a v e s , a n d p r o p o s e d a

t h e o r e t i c a l a p p r o a c h to i n v e s t l g a t e t h e f o r c e s

-e x c i t i n g h u l l v i b r a t i o n .

(3)

233

Wave Induced Vibration f f ^ ^ f c

m t ^ - m ^

m t m

*,15:i±. M^f7t£h\%X\,^?> wave induced vibration ©IfffffiCOTO^©'^•5 1 1 IC, ^ n f , C D H ^ ( D ^ a t t ! C ' 3 V > T s f t f t t l ^ f i 5 l i , # > ' i a t f Ü è ® - : . g ^ l C springing ItgL

I . ft a

2g5MKi*,2.v>i±3|ESCDMÜi=&a;Ts:ii:i5^i.5. rfLe,CDj|öö;MSii»±, ^ K ^ ^ S i ^ t i ® t j M Ü i 19 fc

Z<Di.'jfS:mmmcomm'mLXii, Saunders, H. E. ® i : # " S r f c | 3 i i 5 n - r f c l 9 , t ) ^ - M » t c i.-^xm^iZ^^'^Samm^i-i^lfL Ben and Taylor" JfC J ; T ^ ^ è f l . m # « a i ï t t ±

m^b" fc, ^^u-^ + i f K t l ï l i Ê I - ? . DW 76,500 ton CO f > -izmmU « 3 ^ 4 4 ^ 7 . ^ 7 0 ~ 8 ^ 1 2 H © F ^ , m^). « ©iKWtr. ± m fiïjfCióSöm, midship^üy--) ? 9 S ® ± T i P ; ^ S , «ömmidship^üy--)£cD2 (square station 9% t 9^midship^üy--) IC t >midship^üy--) O l t / i f f i i j ^ - f i ^ ï C i - o t ^ ' üi*ffi, /<-7-,f ^ ^ u ^ t - f P i c i ^ - t ^ S i t g | j S ® i t P J i t - ^ ? T ' i ^ © f ê ^ ® ï S : ^ J è g l i ~ S

8** izmt- mit2, H 3 f c 4 , 0 5 t 6 , mT tsfi<^t\^'n-!^cDnm^^x-^?>.

mi t2i,^i^hi-hi.Tiz, i&^mmi'/\^^\^i,zi,i^i^hh-nmm<D^mmi l o o g a i e ; ± ® J I T 2mmwn!>m±Lx\<^i,. th±Tzmi:nmm^(Dn^^7mmmiy'b^^^^iii^^i:x^^z. ttz±

0 3 ~ 8 iigmtSMfC J; S * 'J föiëS;^ 7 mo±S^itizmmLh'^(Dmm\X-kZ.

(4)

234 ^ 40 ^ lALTtal *' *r vertical accaltrallcn ,l F.R *f VtrllMI KCfnthK tt aSdMp *M xtrllnl accfrallto at AP. 1 m & s :f3, ±. T m

\

% CO E » if Horirontel aectlarallon at r.P.

I

Bottom Prtssur» No.l

Ar Varfieel aeeataraffon at F.P, A* Vvlleal accalaraflon at mliMlp At Varlical tceahmtlon at A.K

(5)

m»<D Wave Induced Vibration t t ^ & l c H i - 5 - % ^ 235

y——^

Ar HoriloMal eectltratlon ot F.P. 70,^

m 4 m^Ê, m m f ^ t m m m o m u

Af Varlleat eecefaraflon ot F.P f ^ 1

At. WrtlcQt aceêttratSon at mfdsnip T el 8

As yêrtlcat aseéftratlon at A,fi fi

0 5 l ö l S f l E ^ I , ± T j t ! q a S t D | 2 g

± T J n a S ( i 2 g ^ | a i S L T V ^ 5 ) . C © l 2 g - C i ± ± T 2 i 5 ® ^ i ! i t a ] l S l ± 1 t ( c ^ t < li'ii^^is, Sffi

a±0i•5''d:S^si^^'^9^*iIll^^ci-p•CSleè^^5ffift^ii!lli springing t^J^ whipping, {5;f3ji springing stress ibSViti whipping stress fcDïlf l a t l ^ S ^ i s ^ f f ^ ^ ® K S V ; i - ' b f l J K 1 " • & tJ)? ®i7lc^l^5J'it-CV>5i'5-C-*)5.

(6)

23Ö

0 6 mm, m m n t M ^ m t o m u

2) Whipping: ïS^-^SÖf*iiÜ0;*C§Vvhè V»Cr5-;5-be>-f, SSWKffi*'?' bow flare impact

'Jfmx\t, wave induced vibration (:Ht-5H-S;iÈt::':>V^-t®ïM^J:¥f5tè®Ü-r2.11 fc 1', S

2. Wave Induced Vibration

springing ^ w h i p p i n g ICJ: SjDnüS. ffiW^® < ftlf * - > > ^ fci 2>'iS^J'i t ' t l t ^ C L f c ^ S : CD£il'ifc®**>(fHl£, s a " ' " . Kaplan e t a l " , Goodman", Kumai and Tasai", Gunsteren »'

(7)

mii-CO Wave Induced Vibration ffS^Sfcl^-r5 237

g a * ' l±Wagner"> 0a^}cS-:^V^•r j | 0 J g » * ® t t E t ^ ® | | S t i £ t c o i ^ - t : ^ i ; T l > 5 . ^Oifê ^ . i E K i B ¥ O i E * ( i e ^ S S Ï ® « ^ ® f f i i I l - i ± ' < 5 - i : * ^ ! 2 f ê a ± f ' i a i - 5 i « , ® « S C J ; - , t S T 5 jK(*S«)t:iSb-Cti, M^f6»(rJ;5fc0:i5m'54r;*:§i/^0-C. whipping ®ISHfc b T l i S f t S S ^ t c

Saunders" ! i w h i p p i n g t t T . « J t S ? ® * } * » * t i a 3 B » ® ^ H ® 7 i < * « W i - 5 # i n H S t virtual mass ® 4 ' T , non-linear (mvir)„ t U, -?;®25^}-0±T>?I«lSSè > i f H l f non-linear tl reaction force F„ |±i?:3dCT-^A iöH2> t LTV-'S- EPt.

f'n=-^C('«wV)„>2. (1) iSöl"0±"F^ffi y TJS J-oSinOei (ü>e t ± ® t ® W é « S a ) , $=myacos<o,t -t>*>-=Tt,

H i s non-linear tt F„ immizm< h\-^^^7Ll5Xihi>. U.S. Navy © carrier ESSEX (--5V> T l t » - r 5 t , 2 « i j g l l ^ ^ U - S S : - r 5 g f i t [ > } ' ? 3 e > n 5 t ® - < 5 1 1 1 H , r ® : S K T ' flare impact ) & : f l c j ; 5 whipping è fc I t - ^ - f S Z t;5>-Tt 5 t l ^ U T V S .

g a " i±, ^©/J^èv^^®èg^^tf:liT)5^^Tr5^ö*^m^*Jli!l(4%^^^^:v^®H^jtv^ whipping

S n s ) H i - : > T S T 5 i I * ^ # i | g S ! t ' t f 3 . ^®4'®2|5MBi!3ai:raUM®:]KBE^J®:^I*«SSilfig:Öf^ ' i S t ^ U T l ^ S . t'S*?*,, g l 9 T » 7 K ® $ WoLo, WL t t S - S f f i f f l ± # i ^ S $

AF=AB+-^Umy) , (2) T - ^ ; i T V ^ S . AB=2pgby, Am^pizbyz t t ó l j i f

(8)

I

238

m

:t

H 40 ^ |

0 9

i<

JV

-f

M

<o

m m

AF=2pgby^^[^-y) (3) hti.y), 7 Hi-p-C b ^!3E^b-t5®-C, tzkpL y=rocx>sa>,t tL-Xl AF izit a>, £W©Sf2^®fig •

X'<jv-fizgi<tl Ft

F 4 = - f - { l + ©i cos cos <!),/+©, cos2a)«< + e,siii ZcDj+e^ cos 4a),n (4)

S60 2 a 5 S i i l S C ; i « ( 4 ) S 4 ' 0 f S i n * > i : - g t t - t * S t n t f whipping iih^. IP*, selective reso-nance |Cj;^-CSfil*>'S5. ^hizmt. ö f * g 10:5 h >®ffi^--^V^T K'=50 h > t L T $ l f ^ L , gegA=30m t 50m ® S K S Ï i r S 2 g S S S ) ® - h T J P a S * * » K S ! M H f i l > ® * ^ X V ^ 5 .

Kaplan et a l " l i , i ^ ^ I I J S f f ö i T S . fiï^®jlii)t±S'^®x K • / S l É T t t S L L T ver-tical shear force, bending moment J^^ft, W3UmWi\Z-o\,-^X\iÈM^b^M^o:>m^l3m^^ m^^X lateral shear force, lateral bending moment ^ ^ f c , ;H?>®jS^§S!K^fflV>-t^;SfllJ&

^(Oj&WMWUzmrf < bending moment Ti fc-®|§a®)tett05j¥%fi^Sft2':Si£$ i•fla3^L-CV^S.

(9)

ma^O Wave Induced Vibration fftgij^ftü-r 239

j',=vertical elastic deflection, c=damping coefficient, V',=shear force, /"(^r,/)= local wave exciting force.

tti r=deformation angle, KAG=vertical shear rigidity t t t l l i

dMtdx^V. + I , ^ . M=EI^, (6) è-C, P(.x,t)\t, # J l H S t t S H J ; 5 f c © § P^{x.t), ^ ^ 3 ® ^ ^ b H i ? , i ® * P^ix.t) fcL-C, P{x,

t)=p,ix,t)+p,{x,t)

t t - c v > s . z.h\mw hmm^sx^z-

mzp,{x.t)

t t - r ( ± . e>:^

P i ( x , / ) = ^ ( m „ t , . ) , ^ = - | — ( 7 )

^ i / f b «/,.=relative velocity=i-*Ö-l-Vö-Co. (8) S)*;, V=fiöi^, Z=±-Ffi§^{Sr, e=im^^, f o = g f f i ^ 0 orbital velocity ®±T^f|q]Sg^^,

=#iina<i#i;pSS-c, ffS®^^i0#^^SS^^f.^*ffi-c^^rv^sfê®#ilIlHgtMb§|v^^^t,®.

L T : ^ ^ S I M 4 ' ® « ö # : i 5 g : ® ^ ^ 5 1 M ^ è i t S b . bow flare slanunmg H i s whipp-ing bendwhipp-ing moment © ^ Ö i J ^ ' f b è fc^ftTV'S. carrier ESSEX .tZ-:3V>T3Slttt^èfTit£-p/;ifê

2 f ï ® ± T S Ü ( C i s bending moment (4^S:^# <^^,HS*<, 3 g f i ® ^ n t i ^ ^ - C ^ S f S i f .

1) mnm(Dm&\i. xmimnm^Mzm-^&s.t)tm\zm.m\z^L\^}iLtz. 2) )fö#:Si&;}iSgïl{fci(i:f^gi4^j^U7^;.

-/,=entrance length, m,=co^o= hhX^Mzè,^nmo'ti1smA, y=m^iS.(0±.^m&-® e . y=m^iS.(0±.^m&-® ^ x . : ^ f c g a " # i n i S Ö i l y=m^iS.(0±.^m&-® ^ { b H i S ^ ^ S « t « : A * % x , selective resonance tr i -3 r ± T M S i * « ^ S è n s t - t s t . ® - c * s .

( i « e 0 ^ f t i ; i : - 3 - c ï T ' j C 7 : 5 S H i - 3 T , g i i i i i i : ^ f c - i J A ' m i d s h i p Hfc^tssi^l^s:ü^&|f|?LTl/^ s.

(10)

240 ffl :t S 40 ^

mmmölzX^xm^Ltz 2^ ^fflV^-C_hTMSifS®co|fi:=£fTJiV\ i89fil!2fcffiO^-(bi:

spring-ing C!>|i^H-3V'>X|iD-Cl^5. È ^ ^ i ^ ^ H i S sprspring-ingspring-ing C07jc<i^^èï5^tV\ sprspring-ingspring-ing ] ^ selective resonance H i - 5 - C ^ S T S i t t ® ; 4 ^ » S 1 1 fc H, springing (D^ckWMMW^Oi^^

Ê l ± 0 | f - g L j Ê t * j S f i ï H M ' Ü f c 0 H , Goodman" t Gunsteren» ; n e . 2 A

MiSfc, P^4^i4fcv^•f*^fc-^i?©S^êl^^tL-C^!6i^ t t- 5 f c® T* , 5 .

CaCOs(*x-ha>.0. Ca=KM«i, *=e>V^=27rA ' l = S a <Ui=a)-FAK "Ci-S.

i='(:c,0=^Wsinfl>,i(ü>.=ttièraMii)|SO t*JSttf, njJi® mode ® S ï I i a » f M « l 0 ^ C ü 5 ^ { i e > :

ü-„Wsin(a).;-^„)]_ F(ï)f/„Wrfic

tztih ï/„(a:) = normal coordinate, A„=« S:®@^i

A = f ^ A ( ^ ) W W r f « = | ^ ( ' « + ' « ' ) f / n ' W < ^ ^ (13) I

C=|^(;V'-K-|^+c)f/„»(x)d;c. (14) I

; r - c w, m\ N' t6iiV= C' {±, S S S ^ i f l j ^ f i ï S è S t J ® ® * , » f f f i f f l ± T S i ö H * f T s # i n S a ,

mzmmimii,

F = r ' ' ' F{x)Un{x)dx

i-Wl

=2P8\y^U,,{x)e:,dx+\(N'-V^)u^Mt,dx+\m'U„{x)^,dx (15) -CJ^itf>n5. i^:/i-L., Ci=Coe-*<'icos(èx+£Ue<), Ci=-CaO>e-*<«isin(*A:-l-o,t). fi=-Coa>V-**J

(11)

mW<D Wave Induced Vibration ft^iSicSS-r 241 Froude-Kriloff ©^j, mZT^tm^mi-^H^HmL^O) orbital S S ^ i J ; ZA'JqagHifcWITS di-ffraction force -CJi)5. la-g-fiM^CS^Js 03 * J i i / a 9 ^ t i Goodman" O - ^ x / i i C T ^ S .

^J;ttf «=2 t f c - i t i f , a i l M 4 ' ® 2 f 3 © g i I f i ( f g Ü i © S ^ f f i f S ^ * 5 V > i i , «ö<***ÏEH*3(tSffi

^h^comm^m-x, :^mmmmmmm ?,m 2 giiig!aiSffi^gK{Gij©iKifKi¥«**i^

Ê t ± © ' < / i wave induced vibration ©ffgCffitiS oH::;«cS!lèn5. fiPt>

Wagner"' ©^^ïf뮫7J<®Sg0a^!C^-?V^-C. x 5 ï > y m ^ ® ? ^ ; f t t ^ f ö » t ^ ® < ® » * E H

(2) ü s i s s i i

mi^K..^piimm&mm&3mt\zi.zm^Et3m:b(Dmtmt®#^ss$^«LT, *®4'®2

m^^^^Zm&WsCOfSMtlbti.. mm selective resonance (DMÖ^mi^^k LTffi{#;g|&êi+ ^ - f S (Saunders", g i a " , Kaplan et al«'. Kumai and Tasai". Kumai"', Kumai

(s) immmizi^mmi^

SJft4i®J8#iSSS®lt»Hffiv^f,n5x h y •.y:/SHJ:-3T,Sfêilt?i5êft{*tl(c radiation force i a i JA- Froude-Kriloff ®^j, jg© orbital ilS,JnagHifc|i1JTS:Ö=è#^L.fêV^fög®S^ïèHS^ • t - . 5 - i ^ H I S S a t L T i ^ § i a ^ H J : ^ T f f i f t g » - Ë H - » : - r . 5 f c ® T * . S (Goodman", Gunsteren").

3. Springing (Dtt»^IC•^4^r(7)#S

itfflitc®--<fc wave induced vibration © 3 a®©|fS!.i£©4'T, springing {r-:3V->Tt4(2)i: (3)®

i<M.^tzibtsi\i^(DX. *6^Tii2'3®ft^iSo^aS(cov^T^ft^èl)[^.^.. è ? > H * # ® B ^ è ® ' < s

3.1. a S K i S S S Ï

m 10 ® * i f ê T g ^ T i 9 i ^ ® § fc-o2ikTt&^m^Bm^M^xmmm yo X y=yosmcot 0 ±

' ^ + i ! : 0 = O , at >=0 (16) T - ^ ^ ?> H 5 - aej ^ T -fi:=cöV^.

(12)

F= - m'y -Ny- pgA^y (17)

-mJ-pgA^y -C^sS. o ^< O X'i> « TfciV^ti-a-. >»' t A^ti <Ü H i o T ^ i b T S i t i i i G

5 ^ ® # t n H f t t n - ^ b T ^ © ï | i ^ ^ è t n t f i j t t i # ; * « e È S M ± T /=o -c,m{ciiq:a*>-5VMi^èn2.:fê-a-li, « = o - r © g i ^ ® * f ^ f c 0 = ,

O httt), ü>->~ ©*ê-i:±<PI«5'i«it<*A*^«ië:, >«' © H - ^ i S t i a i u - r i . 5 .

(«.'>) = - » » ' y - : y - 8 7 = - " « ' i ^ - J » - ^ d^) t - r 5 ^ x > ? i i , K4nnin"' ^ W a g n e r " ' ('i-^TlÉ-tf ^ H ^ c i 71^:, ¥ J È © ^ # : ^ ^ ' * ® f ' S T L

x^mm^^&irzmwiw-t}'?m&iznts^j:}ii±^üm''hè <, motn-mM-r^tLxmi^

i l è * t ó i 7 fcT2.«)©-C*S. r<St/^Et^ra®i^^-Ci5S*><b. g È ^ S ^ f t i 0 = O - C * 5 f c # m.'fc ö » ^ » ffl^-ê-tiautófc'iS. y fctfcH!^<*:©;ïKSti*^iit'S^bT5^1iaSS©^2 ]S^i^sfeT#Tiv^ i © i 7 » ; a s i * f f l i É i i * 5 S , mmmw^-cwmmmLx\i-:hfmm<m#ts m^CO:^mmiT^ ^. g Ö ^ H± - r Ü 5^ S ® S i i! t t 5^ - t . ^ i t ' S i l t f f l L f i ^ t c ^ J i t S S i ? ^ ^ : ^ / © t t ^ H / S V ^ e j f l S a ü T i s S . ïiÉ-:>"C, Kaplan et a l " bow flare slamming H i 5 whipping

(13)

mt^O Wave Induced Vibration immm-tZ-^m 243

li9^mW:X-^^, ± T 0 2ijfêK0@^||fflt±2g^föx-*>S. « } » S S i J 0 » r E 0 ^ b è 10m èr-rn

i f ? B = - ^ 1 " = = - ^ «Ïg§-Ci±0.25, 2a5®±Tfil&-Cii5.0 fcAjrS.

i ^ i - , RfêSlïJ: © ± T S t T 5 ^ i C S r S « t ^ : Ü i 4 , i t S S ^ ^ ^ t l C L - C lst-order,2nd-order

• • • © | ê l ! f e i ; & f ^ ^ i e ! © f f i f t A t L T ^ J 6 5 ' < # - C * , ^ 9 . J:J^©RMiC^S diffraction force b L-ct±iiS:a94'®±TS^fi:èS^fö-c*i^*>^fi.if, ïï<Kö5t;ii5È-cèi 9 .

3- 2- Goodman ö ) S g |

MS4MKi--^V>-CI± ^ï^^èV^Ö-rH^liaéi^-C iV'=0 bi^è, W i ± r ö ^ = o 0ffl$ffiV>S. Z ®IÉXTfflfll^©iiC©itH -^-9—f4'U> : * s ï ^ S t 5 ^ 2 : T j c . S . ZiXliT, h ') T ' S ! : i H i f S

^i±jT5i$sti-c*,5*>. ^Htxmm^tm.Lx\^zmmmmiznLx\i-mtimMx&?,. m' {--7V>-C{±^g#'»''"> ; è : | | i ; T V ^ 5 i 9 i-S&tt:®t3^!-*=-l^-tli3^^JTC^g^Ji^t < , dm'/dx fcjfö <*®SlI^-C#SLft'J^Sg-Cii^t::i£l-'OT', w' © S ^ ^ i c t ï k ^ a f ê - o T , -Vdm'/dx i'oV^-C^-» ® W ^ ^ 5 M i n s . Goodman ©S^fc»:©2J^{c-^v^-ï:Pfgg^5^^,Skl;'5• 1) 2giigSi©j; ^ i- ®p^èv>j@SSc®mT, X h y •fmi^mx^zot^') 2) m S 4 ^ t f ö < * g i ö H % n ^ - n ^ . ^ T S K ® ^ ^ S ï i > - ^ S i - ^ J i : S ® T i f f l ^ è J l f c ï i ' t t p : L i ^ 4- S

Ët± wave induced vibration ® l t S L f ë è 8 ! ^ L . ifêi:: springing ® f t ï J S t z M f s a t W è f ï ^ - o

springing ® 2-3®tt^aHi±^n^:nF4S*ï*>S. *Tfcg|!li,l;S^(± springing © f f g f f i t

L-cii^afiüTitcv> t ^ ^ t , n s .

^ ^ J ± , springing i±, S&fiSil^^TS^Sêftft^Jtcii; S-^i^l»i©^i•^C. ffitefjgltfc t o X

ummw-t\i=i5^^^iBiii©ffl#izi-pT^èHsfc®-c*>5t^it.s. tiÉT:>x-^mm%\wm<Dm^

(Dfzmz\i. mmz-z>\^XiimmmWtHzmti^\~>) v-fmo^^BO^M.

(14)

244 B ? ^iO^

im^=-^'ssLm^i^^mzm.^f>&tmmo)m^^nmt, ttz whipping © n - g : " H ^ L x i J i mmtLxmm^^xm<m^^mz^tii^, z(o/i^m'ki-<^-=i^iftts:-otz. v^sv>s«5iiM3K \,^tz^^iz^sT^-^mi^hmiiKmXÊbi>. ttz:^mzmnLtz wave induced vilmtion ©.OJJ.

# # S: itt

1) Saunders, H. E., Hydrodynamics in Ship Design, Vol. HI, The Society of Naval Architects and Marin Engineers, 1965, Chapter 16, p. 288-322.

2) Bell, A. O. and Taylor, K. V . , Wave-Excited Hull Vibration Measurements on a 47,000 DWT Tanker, Shipping World and Shipbuilder, Feb. 1968.

3) m^rmmn. a f l i « ö " B A " (Dmm^mom^, m^-^m^^n, m^zn, m^iè^^n. 4) a f a s s i . ) i & i s « « ! o K S t Whipping i c - p f x , mmmm^T^^, ^ 3 2 ^ . mfi^i^^n-5) Stmm^, Whipping ^ 4 © - ® H l t : - 3 0 T , B a ï B 4 3 ^ 2 H , a a E 5 i i § ± ü f f i * (ras]48^

12^) icmm.

6) Kaplan, P., Sargent, T. P. and Raff, A. 1-, An Investigation of the Utility of Computer Simulation to Predict Ship Structural Response in Waves, Second Techni cal Progress Report from Project SR-174, "Ship Computer Response" to the Ship Structure Committee, June 1969.

7) Goodman, R. A . , Wave-Excited Main Hull Vibration in Large Tankers and Bulki Carriefs, R. I . N . A . , April, 1970.

8) Kumai, T. and Tasai, F., On the Wave Exciting Force and Response of Whipping of Ships, European Shipbuilding, No. 4, 1970.

9) Gunsteren, F.F. van. Springing, Wave Induced Ship Vibrations, I . S. P., 1970. 10) Kumai, T . . Wave-Induced Force Exciting Hull Vibration and its Response, Hê?JSI6

^ 4 4 ^ , 1972.

11) Kumai, T . , Effect of Ship Side Wave upon the Resonance of Hull Spring, Rep. Res. Inst. Appl. Mech., Vol. XX, No. 66, March, 1973.

>th, S * ) g « ö ¥ è , raSJ44^7^.

13) Wagner, H . , über Stoss und GleitvorgSnge an der Oberftóchen von Fiüssigkeiten, Z. A. M . M . , 1932.

14) KirmSn, Th, von and Wattendorf, F. L . , The impact on sea plane floats during loading, NACA, T N 321, 1929.

16) Potash. R.L., Second-Order Theory of Oscillating Cylinders, Joural of Ship Resea-rch. Vol. 15. No. 4, Dec. 1971.

Cytaty

Powiązane dokumenty

Koncepcja federacyjna + Winston Churchill Koncepcja federacyjna + Konrad Adenauer Koncepcja federacyjna + Alcide de Gasperi (premier włoch).. Koncepcja konfederacyjna + Charles

origin and hope for success. The basic research hypothesis was the existence of a positive correlation between the system of a functional family and the right level

With ellipse cellular design, negative Poisson’s ratio was achieved during the compression and the overall energy absorption efficiency and deformability was

„Poprzez badanie prawdy człowiek wzrasta w mądrości upodabniając się do Boga, a podobieństwo jest przyczyną miłości, dlatego badanie mądrości szczególnie łączy z

Among the three sintering sequences, the module sintered by S(a) under 30 MPa pressure shows the lowest von Mises stress of 63 MPa on the

Tablica 5 przedstawia typy zaburzeń preferencji seksualnych w postaci dewiacji seksualnych (parafilii) oraz przed- stawia dewiacyjne zachowania seksualne lub zastępcze

REScoop Membership Factors Favouring Household Engagement with Energy Conservation Behaviours Whether a REScoop succeeds in influencing its members to set energy-saving intentions,

door de samenstelling vna het Eas. Opgemerkt dient te worden, dat een hoge verbrandingswaarde niet voor alle gevallen waarin het natuurlijk aardgas vervangen moet