1. 3i8£te * 192-9 mm&f-s.
— . c P p m x t ? > Hit-h;u?cDttiij—
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H IE ft**,
lE^ft ZE & IE :?§*** IE&R <h ;ir 31 — ***
An Experimental Study of Flow Around CPP Blade (3rd Report)
Measurement of CPP Blade Spindle Torque
By Masamitsu ITO (Member), Shosaburo YAMASAKI (Member),
Masamitsu OKU, Hajime KOIZUKA, Masahiro TAMASHIMA (Member)
,and Michihito OGURA (Member)
The hydrodynamical component of CPP blade spindle torque that plays an important
role in CPP design, is investigated.
The hydrodynamical blade spindle torque of two model propellers (MP. B 82--1 and
82 2) was measured by the newly developed support-pillar type blade dynamometer in
circulating water channels.
Measurements for two propellers in the uniform flow field indicated that the
maximum value of hydrodynamical blade spindle torque occured at the maximum
reverse pitch setting and near the bollard condition ( / = 0 ) and the dominant factor
influenced on the hydrodynamical blade spindle torque was blade contour.
Fluctuations of the hydrodynamical, blade spindle torque of MP. B 82-1 in the
simulated non-uniform flow field with the wire mesh were measured. Although means
are much different, fluctuations were nearly same for the pitch setting angle from-10
to 10 degree. It is also seen that the means in the non-uniform flow fields were a little
higher than the values in the uniform flow at the same operating condition (same thrust
condition).
Comparisons of calculated values by the lifting surface method and measured values
at the design and the maximum reverse pitch setting conditions were made and they
showed good agreements. Then in order to use at the early design stage, spindle torque
estimating charts of AU-CP series CPP were drawn based on the lifting surface
calculations.
(CPP) sM±cDjKnfc«j:of^«E*, m
vj~-fv^v yxh, b*? o^mmwM $ ti ^. CPP i? i±, c
81
4. o
j^m^x iyy%m^mmytz^y]fL^, m^ycx^ A MAXIMUM
CO
o
o MINIMUM
X . I f ^ i ^ P - p p p D p ^ ^ ^ b T f t - b g ^ , .xb CN
P KP b P 174b oElt5lE{ilCDP^4r- P P l f S l t ~ o
o
-4
A
O A
i.
o
o-
o
OS
o
8 0 1 2 3 4 5
SIDE FORCE, Fs, kg
Fig. 8 Interaction on spindle torque output
due to side force
U-4*- b ^y~l5^my)MXchy>* Fig. 5 {C^IIIfcg
ffib^ffetJff (DFB-12) £ , Fig. 6JC|fcbf|P7^B
/p/b 4 ftCD^WigScOXiS^^- 2 ft^ogiif $ t l f c p
F P - P P - P , lti64fcJci:oT||'ffl§ns. y^^-y
Ffr bfr? %$:#>% Ki±, PCD 5 hMt$t~ &&&&■$:
ya%(D7 b p F ^ h fr>?%, is * y b -fe p # - a> e >
62, 3 m £87. 3ramCDigf $ (MP. B82~l C 0. 5 R t 0. 7 R
m D
fcffls) ^ i t i ^ ^ i T - f : . Fig. 7 {c^arflis
Fig. 6 Blade dynamometer with measuring
blade
imm i ®VJXMJX$> o ^.
P ^ 47 h -k P $ -1» £ 87. SmmCDffi § i c ^ o t ,
> > Pb
o
o o h = 87 3 rim
> F ^ l ^ c M l l ^ l g j i ^ - ^ ^ T l ^ S ^ I K b : . ;b&-^
A h = 62.3 mm /
i
p ^.s^fq]*^>(b§^, i ^ » > « ^ :? m/y^y>m%m
A
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<->
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{
g. c j c ^ b x o . oejgppb y> tz.
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wjmom^mmm^ t t » ^ ^ 200Hz X$> *>,
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/4
8
SR-171C «BS 10, **ffe^EH-bft MP.B82-lb,
7
A
i
SR-174B4 mmn)%%$MLfcVtz MP. B 82-2 O 2 WM
{
_J V Om^iytm biz. MR B 82-2 ^MH±CD Sftn^llS
y bfc MP. NO. 0661)2) tmmtXh Z>. Table 2 JCp
o
o
Q
CN
Ky x2^yOfyt^7S^,
p ^ ^ C D g a ^ , Fig. 9
2000
-4000 -2000 0
mm*, gfi*B*soHB*sftffaffcD0 2 0512
SPINDLE TORQUE, Q~
7j<fi (SOT^^Tfi;, § 3 x f i X g g 5 = 5 . 5 m X 2 m X
Fig. 7 Spindle torque dynamometer
lm) ^5j:^®4[H]^7Klt (S8!l8PEfi£, S ^ x f i x
calibration
84
9. ^QSH
b
H/D
1.0
5 /
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C
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quot;quot; N
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b Pf
,9 = 0 ° 10 /
o
quot;
^ ^P
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quot;^:
: /
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/
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/ 20
/J
;< ! MP.B 82-1
-40°
^P MEASURED
o DO CALCULATED
25 /
//
s MEASURED
DO CALCULATED
30
/ /
-0.6 -0.4 -0.2 0.0 0.2 0.. 0.6 0. 40/
L „P 35/
ADVANCE RATIO, J=v /nD
5
/ / / 7
Fig. 20 Comparison of measured and
calculated hydrodynamical blade / / / / / 55/
spindle torque 0.8 1.0
PITCH RATIO, H/D
Fig. 21 AU-CP series hydrodynamical blade
my yy yim^mm e nx t b . yyy, FPP C
> D
spindle torque at design condition
W:Mmu<D^^t.xmr^^m^^ftzm & i s § nx
lb13).
*QSH
i t , cppoymL^yyxyjyoovmt, MJZ
isb y yy J< o oVlM®$$fkte, yy^y ojffWjlj -3
m^MteizlLXJk < fHTP b . Fig. 20 & MP. B82-1 -A3
-4
i MP. B82-2 I L O ^ T , 0-0°, J > O 0 i R j S £ , IS
x
b b 2 b ^ P77f|4|3^b 0 = -4O°, J < 0 C 2^M(D t D
ZlM9) QZyjayKy bffibJP ^> bfr b fr y OW3M -5
/
l l ' f f i b b ^ l f i b b b l J b b & cDT*#> S. b b bCDKH
^ S b f c b M i P ^ ^ ^ D i a b . gfUpxbp FP- h ^ ^ t e / / -6
0=-4O o CD^A^i0A'fi:O^, 7f7$gTte7FbTP^
/
I P P 7 p[£lb M / ^ f C b t e ^ = 0°TCD*fiS^>A
/
P . MJjx t?> yfr bfr b 0 ^ 0 i l H b b T t e , P b
/ -7
p F^$tw>bCDi£gii^>stp tuii*[jiiaacDi±bi^? &
-pbim &mtmx<DmRa&m<tezckfc£z / -8
lyyjyL^oy^ity^^hii^- ^ym^y-y^x^}
/
MAU MMX)> burst type 1 0 P H ~ f b b b ® i ^ g ^ ^ b C -9
/
^ P t m t b T b . (MP.B82-2 b | @ f i b : M P . N O . 066 / / -10
T*teHijjfsiasR*(iii^iiA?fflssn^) iztzb, m$^ 0.6 0.8 1.0 1.2
PITCH RATIO, H/D
yyxyyyyytz MAU MMA^CD y y yicmxofr
Fig. 22 AU-CP series of 80% reverse pitch,
omL^te-y^yyytey. hydrodynamical blade spindle torque
ISmLmixy^iiizy: o tc, Sffi0iSlilf»S at bollard condition
PteP<P7)>b)Klii^^lletiTPb. b*>U Sit
gpgp^PT, (i)f$IS®S:oDiSo^3+b^p, tatfffr £ bb>T, ff*KiSgfTte«b03S^hCol^TIffili![-
%^m%x§ hyy 7b^yyymwtnWmmxiiy. b
iI$Vcll<7 b C^(2)^bl 7 i : 7 F P h fr 7 CD^*fflt*>S
fffiM^SrbbPbp bfr bfryyii&mSix^
bcb^biSxiMb^p, ^WilS^IScDttm ic*5tf oM^
5 1 ^ 7 ^ 7 F P h^^0||K)£bc^/rfflii(cte-b^ mt,ny>.
ftbtibbfijBibbib. yu^yyy^^itk^oizjmtbx^, jfrmmmm
— 89 —
11. i2) mm sb LSzym^ ±Aib*: b n ^ 7 / ; b iiBm%^mbizxmmmojmmkoymz,
tb^im, y-7 ey--73 7jkiimkt}( WL
D Byy-ik§L^^mxm, »i46bh PH54. 12, I P
■fifPlb H # i t M S # , ^109^-, BH56. 1, 73
P. 20 15) Yazaki, A. [Model tests on four bladed
13) dlllff JEHSb H I E * , bbjliib*, S b t l l ^ , controllable pitch propellers, Report of
fePTtblit^b JlSfi^, mWiMM : Highly Ship Research Institute, No. 1, 1964
Skewed Propeller <D ffl% ( ^ 5 ffi 3,200-&S 16) # i quot; I i ^ * , O^JEHfiU, H X * : AU-CP P
& gS/^7l^i&^0^ifJfiJ) : H * M S ^ M l i * ^ 7 # J 4 t t f g c D S S : S ; * ^ t b 0 b p P 7 |/J»J
3C*, ^ 1 5 3 ^ - , B858. 5, P . 163 ISft^OJEffi, H S 5 t l & S ^ E , ^ 1 8 1 ^ 7 US
14) Hffllbgb HW l b inH^? &, fjffiiEPPfii 56. 6, P . 25
91 —