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Drgania skrętne - Modelowanie

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ProQuest Number: 27591595
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m m a w Fiom m mo piATss
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eoted upon eeueee I t to m>v# peet It# o rig in e l p oeltlm i eW
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v ib ratio n reau lt# from the frio ti< n m l w elatanoe exietlng
in the eyatmi during the motion*
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3
vlbraticm a çan be dOriymd from Bewtw*# aeetmd la # *
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d iffe re n tia l egwtl^m o f m tlm Wme the fern
am = #' k%
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e la t i / 3 ^
end
eoe tV k /%
ow
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tlone vhloh reoeat thew elvee eeo^i time a fte r an In te rv a l o f
time
T * the period# eu(h th at
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or
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(3)
V k
In o r ^ r to determine ihe oonetante o f Integration
aM
%
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f lia lt e iy
at W
th e W
lt ia i
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in ltl(d mommt# W
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ma## la palled oat o f It # poaltlm i
and It# In it ia l velo city 1#
Im aqoatlon {2) glv##
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dz
A# the velo o lty
% * ------# a t
t » 0 *
#
Baao#*
dMk
^
0 .=
aoabtltuting o f W # a raaalt# In equation (2 ) lead# to tb#
a i^ r o a a l w
^
/|g '
m = — — gift t r — # % 00# t4'uM
V% &
V m
*
(W
Otherwl##; I f the maa# i# palled out of It# poaltlom o f
aqulllhplam to
%» %
and W m mleamod wlthoat W L tla l v#;^
lool% # the fo llo # l% 03q>ro##lon fo r tW vlIxMitory w tlo n o f
the maas v l l l bo obtained a#
X a %0 oo# t / —
^
t$)
m
iEhl# apoolflo iB^latiom repreaonta am amda*##d free vlbratlom#
o f Vhloh Iho period# maplltade and It# natur# o f movawnt are
a h ovm I n
F l^
2#
7
X.
*2^A
Period ^ #
m d % e jW k liW d #
%o *
It 1# mwtomory to denote
4% * e$%loh 1# W m m
me tw nmWamI e lrm la r freqnenoy #md 1# memewed In rmdlmne
& # reolproeml of T le defined me # e naW»
per eeoond#
r#l freqi^eaoÿ^,
In eyole# per eeeoM# end ^ivem by
% n r
if
|îT / / m
ü
h
e
m
m
x
i
m
m
d
l
^
I
m
o
e
m
e
m
t a
i
^i
e
% e w o l-^ a t o f t w
nm ee
m
im %
m
a
p
l
l
t
u
d
eo
fv
i
b
r
m
t
i
O
R
#
# m@d $ h e m tm tle dm #
flo c tio n of the eprl% under # # metlmi o f the w e i# t ie
%
cT»
mt
k
W im m
k
s
m
cfl
R
r
In
mt
In e h e e a n d
g *
3 ^
ln * / e e e * ' $ # ie
m l fm q u e n ty # 1 1 1 b #
1
jê
f
^
or
2T
2
T Tr V:/cc Q
C j;t
fn = 3 # m V î7 3 T Z
<?}
SMm mlmtloR#dLp ie very uaeful fo r <^ek em tlaating
tk e m t u m l fm q u e m y o f e v l b m t lw
a ym te m # ie n
o f the vlb m tin g ma## 1# kiimim# and
tw
# e l# t
a ta tio defleotlon oan
b e e a lo u lm te d f
1*3 Bevi## o f Tomlon % am oteri#tlo#*^':'*#% e e la a tio aefor#
tm tlon in toreiom of a #haft m y be derlvea frcm # tr# i^ # i b f
mmteriài#*
Oommiaer à o ireu lar ahaft of aim^eter a
g#% Z # being WLated by a torqu# exiled at m e
* lenr
It
earn be ehoim tb at the e ire u la r meetion o f the ehaft remain#
m#mn^:5ed In #11 It# dlmenalem darlRg the t# l# t; provided
tim t the anr^le o f W l# t 1# very # m ll#
ta&e dia ram ^o#a in Fir;# 3# #ie etmln 1# given
1)3^ th e f o llo w in g
e q u a tio n #
« ---- ss I*<p
dx
i^ere 4^ Im a eoietont denoting the m le of WLot per unit
l%zth of #ié #mft*
dx
U -rdB
% # 3
%0 etroaa
a =
Wiere
% e T o rs io n o f & S h a ft*
# # In Ibe# per aq* In# # la f;lven by
G /T
G 1# t3:ie *m)dulue o f rig id ity In lb@* per aq. In* o f
the im to rla l o f shaft#
a: = 0 r 4G «
At the aurfeoe o f the eaoft#
Or
dx
Gd
—
2
m
(—
dx
•3
Wm? Wm s i f f l e t em&
£m?m i»
sââ »
#m@ taj® top#» aeting «pon t W #afI ts$
=J Q p f^ ê M . = 0 ^
T
Itoting # #
J m .polap wm@R% of ia«pfela of oposs-ssettca»!
« *» » 1 » Ia J * ‘
Ve^m
For
a -eipoBlajp abaft
a
n
â
32,
f »0
«
>
J»e
<
0
(
T
T
#
/
3
SÎ
T h e r e fo r # t h e r e l m t l m
W W em
th e
e t r a ln
#md # #
e tm e e
o f e W letlx;^ Shaft w lih in the lim it o f p ro portionality o f
#w m aterial la #ven by #ko follow ing eapreeal<m#$^
T
«
#40
m
OP
S
J
2s
= — -
(3)
&
&
®
f
e
o
p
a
i
e
œ
a
S
.s
p
p
l
i
j
g
o
o
n
a
t
a
s
f
e
o
pt
f
e
o
t
o
r
s
l
o
i
m
lp
l
g
i
-
9
a i% o f tâîO Wmf# Is
«a # * to *# ®
Is weesm -
sgy to ppoâoc® as aaagl© o f tw is t o f # a s h a ft @#ml to oas
» a ia a .
Hiwj®* i f i t I# d s n o t# b f k% » I t fo llo w s # * t
f
m
ss
@
F w
m e ir m l a r s h a ft#
I
J
=
7T ^32$
ird A a
mmmmt o f im ertla o f a ro tatln ^ body 1# a mwsmm»
o f It» propm*ty to ro s la t m y oWmgo In Its moMon proaioed
by mtomal aotlom*
It la# im ^'onorol# e x p m m W by th#
Integral#
V
Where
g
dm = me## of eleiw ntary p m ### in the body#
r = dietonoe of t^ie portlolo from an azlo about
# lo h I t 1» rotating#
3h m m ln a tin ," th e aW vo In te g ra l# I t 1$ u m m lly o w v e n le n t
to met
I 5
g
^
in 3b##min*.©»ee''
#tere r^ Im ealled the radium o f gyration end Im defined am
the dlmtanoe from the mxlm o f ro tatio n a t ehlsh the en tire
mmmm o f a body %my be e o n e m tre te d and e t l l l have th e mam#
mment o f Iw r t la a# I t ham Im It# omtnmliy dlm trlbnted fowm.
10
If
aadLm#
mozmnt o f In e rtia o f a body# # o u t a oentroldal
%o # i# knmm* it# mmwit o f im r tia # o u t
#%i#
p a ra lle l to the oontroidal #%i# m y W oal<m latM from #m
p rin o ip le o f p a r# ll# l*# x i# thoormm*
I
idler#
=
%
*
I t a ta tw that#
« 2
(n )
d i# # « dietano# wwm m thee# Wo axw#
%>r#i<mal Vihration*^*^% #a a shaft# fixed a t w # md#
ia W i#ted by applying an
torque a t #ie fre e end#
e tra in mergy i# fb#arted in the # a ft#
# ith ln We lim it
o f proportionality# only a very m m ll amount o f a tra in enM
orgy ia abaorbed by frioti<nmO. reaietanow during the motion
a fte r the load ie rm ored*
ed in
The greater propw tion ie etorw^
shaft ae en#pgy o f vibration*
Thi# energy ie av'*
a ila b ^ fo r expenditure shorn the torque ie remove4^ wad tW
torelcm al vibration# o f the ^ W t w ill be produeed thereby*
Oonelder a #l3g#le torsional pendulum# eonaieting o f a
length o f i^m ft fixed a t o%%# end and earryiiag a heavy disk
a t me fre e end (Pig^
i f # e d i^ i# dieturbed fr<m it#
position o f 0(p%ilibrium by the application o f an axtem al
to%*que and then releaaed# toraional vib ratio n o f the shaft
and the di#c w ill be produeed*
In m i# oaae the equation o f motion o f the ayetem
11
b#
by
# #
m m w t o f tW
r e a c t in g f o r ^
00# acting %»<m the # m ft to the re sis tin g torque owlns to
tW In e rtia o f the dlgdc#^
Por w angle o f tw ist
9
dur#
Ing vibration# W# m w m t w M ng on tw #haft 1$ #
hm:%e# tho oquatlm o f motion boo^mms
I ê
I
«
»*
<W
1# t w mms mmmt o f In e rtia o f th# ai#e # #
rospoot to mo axle o f ro ta tio n and #
c o lo r a t i o n o f # o
d is k #
1# the ang^ilar #o^
T h l# e q u a tio n r # r o a e n t i n g
th e
to r ^
olonal vib ratio n Is soon to bo the onalogno o f mo llw a r
% $ * I|.
1#
T h # % n * # lo n a l Om M Do r e o * o f % o o d < m % o t # L
B o # T lm o # m k o # # b o o k *^ T flo % ^ tlo n P rb b l^ a s # * *
MuKhers re fe r to m# Bibliography a t m# end o f the paper*
12
B qm W Lon (1 2 ) h a # th e
IW
e o ln t io n h m
9%) s
0
wW n
m#
###
t » 9 ;
9
»
#w a# fe r n : a #
fo r m
a # e c p m tic m
( 1 ) * hem e#
(ÿ)*
% ## I f
m # d l# p l# # # m m t 1 # *
#0 eo# t
/W
—
(3 3 )
m tM sW Llar wy# # # period o f tm w lom l vib ratio n w ill
b e g iv e n b y
2TT
f = 7 - ......
V %
II
. -
= 2TT /
/ i'
a
n
d
m
#f
r
o
q
u
o
n
o
yi
#g
i
v
e
n
b
y
^ ._ L _ /5 :
s rr J
I
( ill. )
®sis # 6 « 8 # ta t Ap@qwen@y o f t» s is a ia î rlb ra M o n is
independent o f the m p lltW k» but a fu n o tiim o f the to M io m l
s tiffo o a o #
I *
k$; # and th# mmont o f in o rti#
v ib ra tin g m###
I t i# tmderstood from provloua review , th a t the tor^^
sim m l e tiffm e # o f a o iro a lo r s h a ft i# d ire c tly proper*
tlo im l to the diam eter to the fo u rth power end invm m oly
p ro p c rtio n e l to the
o c
o f the a W ft* l# e *
# /
I
(9)
The me## moment o f in e rt!# o f the di#^ i# d ire c tly proper»
tio n e l to both the w#i n t end me square o f me M diu# o f
13
grratlon; l.o,
I o c
Benee I t
^
(1 0 )
be o&nG%#&od th& t & ayatea. cem &latlng o f &!be@vy
d lak attached to a lon$ aTondor ab& ft a l l l ea&eate v lb ra *
tlo n a o f #uob low er froqueaoy; g b lle & ll^ b t dlak G arrled
& abort a t& ff a b a ft w ill v ib ra te w ith & h i-h o r freg aew y*
a
8*1
v z m & T io iB ,
1$ $# g#a**#to#a that
imay be
eae#wüwKS ial#% G % t «aadW üby&dPeree bg& % B U ürb& b& ed o a & y tg r 18%*
*&&*%&* fo ro * ladaeed &n t&# eyataa*
%be y lb r*tia & #%&#
a&w&tadknedl le :ped&&r%H&& 4%> ae .f%q&e cnp %#ü&83#& IWf t&w* iSdleM»
i%io%w&I 3M&8l8taaa&e 4K%aj*Sli%5 dkapiiyg t&wa
jU * eàwPuBW&& 1%>
ba ae& llg lb le,
1% or&er te mtgay toreioaei vib#*tl&&e# I t la advladbl#
to
r& a & e e tb #
a & tu & l a y e te m i a t e
« & e q u iv a le n t a y e te m #
la
general# any &##&BgemeBt o f rotary maoblBery found la eagl»
nearing praetl&e eaa be reaeonably traaaforma# In to a alar la *
ma#8 o r maiti-ma&e torelonel vib ratio n ayetem#
%be#e ala»
p llf le i eyetema eaa be tboroa0Hy an&e&eto&&
to r iiy worked oat on the b&al# of the theory o f vibration*
IQy ualBg the an alytle method baaed on the theory ooWblned
sdUWb IjWb&rajx&ry 03> fladül eagwarlBWHBta# i8%e ao]bitl<8& o f id#
%HPGbl«aa ean %»* a&w#a#aa#%fliy (^ytalüw&â*
:8a the ]pre8H8%t obwg>*
tw&r# ia%8 jhm dkLaeadb& la <%f tamaatdbyg t&wa iMH&asMwl agnateoa; alJÜL
%M& dé3pi9i&& @a%& <%L8e%w@*edLk
2#2
Oae*aaa8 ayetem,*##! ayatem eonalatlag o f a alagle dldk
attaebed to a abaft* aa mentioned In the prevlona a rti& le o f
Ig
reprement* the simple
sya&ma
i3JL*%r^Kps;%%*dLgCl gM##LtjL«Ka t&L&adbi llet **%%4K%gp%*aM*#*ia)%t
Î&) *
iab*k
3WWB*#
lagr <%aaa IbM»
( 1%)
][ it 4» 1&%4» s; 0
/ / y / '// ./ ' / / / / / f / /
&#
IBkwe iBogp*»
3/atem*
I0a* ir&b#rbloKi la j& tuap#
aacw&le laotdkaa* Bbw; a#%dll4MLtl(m odP t&w# aK&dbaB%&@#& iBg&adka&**
%aat&w»& 1K&11 fc&sa a lyargr BKM*gGd%&I 4boo& ftor asKlviays t&%» idtbn*»
iüLoa 3pro&>l8BüB*
%dyb tcwa irl&aMktos*r
%w*
#%a #w##&l&a
# # #a a la 4 )a t
I t fo lia * * th at
e
#
at
4%*4A a a la *>%it
# 2
t%y
16
tÈ^ss ia te
(13)» I t glvaa
«■ 2 Éü^ 0 <*■
= 0
ï t la aw n th a t a fta r
i'sS)
usa o f &##»'
Oaaeo smiWd# # » <Siffs»aotial a#mM.oa o f rastlon Woœwm a
sfepla algabrai# © ip ati*» léiidh ®an bo soïw d by m M i m m »
tio a l troaim m i#*
BVom équation (Ig )
a>B -
mâ
fL
*
ï
----- " /——
2 T%/ I
ghow&ng tb# value o f k% * tb# êprlag @#8#%#at la tgeai&a 4%f
thé eb&ft an#
I # tbe maa* momeat @f la e rtla q f tbe dlak#
ta%» %%&tw3%& iSpeqpa&nagF éawi be fowBid jüpom 4&guwK&&c&i (3dS).
3#
ta# BW&aa <%f @8&aft :i@ %%>t sgag&j^&ibika* ia%* i%t#ua%c& a&M&gpKM%ey
edüLl IBban (ïGgH&Qd aamriüky cm t&w* aww&6 swamwM&t <%& iiüKPtdUk oüT
18%& a&kKft*
*%xp tÈw) B8U&* sdT düu&ft %a%y T&e aww&e !%y
iwükli%s laübo aw%B#%8%t 4Èw& mBw&a 3#%m9&rt od* laaMrtlaL iof lQae <&l8k
tG%9&tkwKP %dU8& %8&* 8KW*8 BBameKdb o f iQ#B4&i& <&f tÈwe s&wift jb%
SMülTdbyg t&w»
ilt baw* bewüB aüü&ted 3%reidb#w833r thadb
aeuM&ed au* t&w*
magr l&e 1M&»
<%f d&aw&&p#tjüog i&M* *t8%&&a <w%argQr bap**»
t%> &# aau&GtdUa aysüWKB
au* dljTbarbedb
It# &or^KLtlo& <%P cKpalIl&Bü&Bm
3BT #&&3w&t&<8& il* aawnamedL ibD b#3&&r8K#dl*, law*
jbüKiüOKKgr 3B&y i%& fü%8%& l& *t *lB@du&]M@%#BKr ftü&a enar y oooudi#
4&e**U%&08ab
3h iWba ftüLlasdayg awü&egüü&blc# 18%»
<#P tb#
SB&&8 dur aTàil: w lIl tH) ta&dU&g i%ü%> meaKmant#
3A&P afiiüngie <%f todU&t
b&eqww» &m
tgr d#
<t%r%%y2ipih%Mdk&@& 18%»
* %B%& t%w*i9or& <&%&& (%i :LQAB%ww»&8# 18%» tmdUft
i# *&%&&
%&%*&
#
%b# %%»G#atdW&l eowBnsy &%%the a&w&ft
*w& @«w0ü» *
F.S» - J
k$e. m
a»: klastie ®ne?®r .#
&#
= - ^ k ^
âmstmmt la
K*B* s —— iJtl?
2
#%p@
la the
w lo o lty
Aaaaja® ta » r» tio n ts b»
as
# ■ ô® s in a)
tb «
^
#
“ i r
“ ®o^n®o»«dj,t
d#
a
»potanîstîkl m
a
r
g
yt n
s tra in a w % y la
iS m
& xM v«m
poalM on oj? #
»m a d m &
i
.g
f.B ,)
H
2
h
©
k
im
t
iem
e
r
g
yis
n
m
t
m
lp
o
s
l
t
t
®
»
t
h
ev
o
l
o
*
e
l
t
yiss
a
s
t
e
a
a
m
o
s
i
as
m
a
l
s
to
f#
i
@
k
i
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e
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.
®
m
m
r
g
yo
f#
#
a
b
a
f
ta
n
a#
m
to
ft
b
sa
iA
, 1*
0*
1
2
L
2
IB&e
% 4 a) I
ad»
*&t aagr
<%f t&w* #hadM&
iWbrqwygi liw* le%yÿB& 1# ipro%KMPt&dRMüI $e 8b* dL&ate&ww* f^xsa t&wk
jr&%*d 4##d# 18&* a&yg&lar TM&lowdkty *&
% jRpomlBa#
md m wt b#
=
Urn
I
IBs* Idüa&tjüB 4*G*#%gy o f aw& *]k8a#at <%f lÆQ%ÿ8b (be , cLKataad) %
j&pom i&y& fljB&d dw%&* dkBw&tliyg I@ i&a t&w* iB88a&T8 of in@%MKL&
o f 18%a VÈWÜL* a&w&ft* 3U»
2c,»3s» ==
jk% )
2
6
^
6
jawod IB&we iBCUbatl, ïdjOK&i&&<& ewGSKpggar <>jr 8*%* adbu&jrt; 31» IBbwami
E*B*îïÉîa«s *
2
6 *' o
^
m
IBbdLa;
IBbwadk ta%@» aaawKa saKaaBBi&t <%f jüo*%%»%aiai <%f lïkw» «GaawEMk la*
iagrGMBBs&iaak&jLar #*qpajL#%*]Le&%$k ibot <*QM»**tl%3Lp*& 49#
awüzaa jWBX%taod&
4&%k jESfdw» aaacl oüT tW sGbwajrtk*
]&%
%
%
» (l iG<>KU@4Ke"*SktK%1P# *%yi»t%8S0# 1ÜÜW99P4KZ%%ee%,
aL\,» "
3&#3%4i )di8%s
% erefor$j
à .j= _ 3 *
%D * V 3
&
* - T = - /—------- — r
(%o*QSM83xÊjaag G&K&a; iwdLiaai tas*» 8Kfw&t;&9& (3k6)*
(17)
31» (üGMfjLoRaa* lü&iajb
ib&ü» «Kfyr&olb ûdT 6&%e aseuBB; (OüT a&aauEMb aawssr t%k IbadkBBCk jLK*t%> i&oqpo%*idb*f
iWr laahBw&Nwsfirgr, isgr atdkSjbcys (:%/\)) I*, 4%o 3^% jESap I jka é*&*
oulatlon*
As a g eiw m î r a ie , soggeatM ï f Wilaom,^ the ma## o f
:2*
2kBM) laym&CB&t# 1)€W3&E*
20
i&C tb@ l88g#&(ür
the a&wd^k 3bi fe a t aaajd#üUb&& Tby th# i%%N#WMagy la vi%#mddkN&*
p e r a a e o n d ê o e # a e t &%&&&&
2*3
1 *0 0 0
*
TgowObae ayatam#**» & almpl# tmowme##
ijL j* !> * (K%B#jU*t#
eaw&i oüüL
9L SLangÿWb odT
dbeaa &&
idlth #&]ba*Rry cULak «dk
]&& t&UL* 4WW&G* akf tÈM» ai«8aa @&%» a#üf@a 4t&ap]WM#**f
m08&8 &n o#ro&&to dlreotlon* eaah othar ma& th*& rel*a@#&*
th# ayetem w&ll b# pot la ta & #%&%* o f t#r@&8&al ?ibp*tlo&*
# lg t # ^ 3*0 ^b*o 3y#t#m*
equatloB# @f m&t&o& for th* ma$#e@ 1 &#& 2 #ft*% thay
are glvem a ai8pl8aom#n& o f
6% «ad #2 * roapoot&voly* &*a
b * g& lttea a&*#
% ®2
*
Ô% » ■#2 î * 3 bÈmc O t
♦
%
*
ftj. > » 0
25,
üaiïsg fcô
fowa#
2
f
3 = 0
S w matüpal fr@#iomo% mmy_ %» fmmd ft*®a
(13)
â é ts m te a a ta l
swpatieaî»
k% •
% ui ^
• %
» Ig
'- %
(19)
anâ solving ît j
1^ IgiW ^
*
kjjÇ ïj^ *
Ig 3 ® Ô
(19a)
5
M
al
at
o
©
m
m
#
@
f
v
a
g
w
m
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quote from & ll#o n*3 book, itu a a y be concluded th a t**
I& oaoo o f a d l^ c t*c o u p le d e*oobilcm l
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are several equally epaoed minor m&a#e@ connected
30
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eet# the erro r introdueoa by reduelng tho aotu&l eyetem
to a
or
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3n&I)
;&& @8gr. QaMp&na&B8#&t (%f
Tdübrâdü&on agratWB& tbanp*
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beteeea m%*»eo,
Thorofbro, the tBD*no#e frequency ean not
be obtslnod by the
methodz ##& & th#8#Mm&#8 &y#t*A
will ]&ot enàblG the fr^ tenqy wltb:m&re t^on two node# to be
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Beelde#
tb# Bbre e&aet eolutlaa o f tb# frequ#B#&e#* I t give# the re *
la tlv a amplitude# o f vibretloB a t varlou# ma#@e#* on Wbldb
the determlnatlom o f the vibratory etreaao* o f the abaft
ayatem eaa bo baaed#
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tom 1# &# abomn 1# Pig* 11*
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found from equation (30)*
modoB o f n a tu ra l
oa:y bo
3,
]&%#%&&& ]PR8QK8;oi o&&aa&A%ic
3*1
GOB#*#!**"- Tb* tb # # r*tl*a l **lcul&t&&n o f o a te r*! fe»*
guanal*8 o f
tbe
a&opl* ayatem ha# &##a alaoua»## &a
dbapter#
However* tb# o e a lll& tla # eyetem*
o f aotual lA B tallatloB a *ro oeBAlly laAdbsaore
a# e ffe o tiv e method o f atteok &a aeeeaaary*
&m&
3b f*@ llita $ #
B atural frequonoy ooleulatlOB#* 1% la aeoeaaary to red&e#
tbe oogplea eyatema to aiq p ler ags&ae&emt ayatema#
I t la reqo&ped th a t the #g&lvaleBt eyatem eetalaa a*
oloaely a* poaalbl# the el& atlo and dyn&mlo dbaeaoterlatlaa
o f the o rig in a l ayatam#
E&pa#l#ne# and jud emant In fl# *
e&oe the aeouragy w ith ablob th# egolvalont ayatma
duo#* the v ib ratio n al obaraoterletloa o f the o rig in a l ay*#
tern*
%bor# are three type* o f equivalent myatema being go*
n e ra lly followed*
One type o f equivalent ayetem la obtain*
ed by eonalderlng the moving maaao* a t eaah onmln# oyllnder*
flyw heel* altern ato r* propeller and other la r # oomp&et
p a rt* && eonoantrated ma*#ea ooBneoted by el& etlo Ohaft* o f
n eg lig ib le ma**#**
Rhl* cono*ntr&ted*n&8* ayetem la e%*
texalvaly dlaeuaeed In W lleon** book# the explanation and
m
the preeedwre me&tloaed la tb la hook w ill h* folio####
3*2
Pbeghamey 3bhul&t&&D*~~* I t 1# tb a e re tlg a lly po*#&ble
to fla d am many natural frequan&&e* a# tba auWber o f *p&a*a
1b&t%&&8%k :mau&8#& of i& 3&iltdU48Kw&e agratwaa tqr t&%& 3w&th#M& odT awrt*
&$%%& %#) a jgrosgp c%f &K%aogp&a«K%&8 <&gwKKtl<8%*
aK>tlam jhwam
tkw* f%M&qu*B&Ggr i*qpwKtiaH& awwa t#» dwKP&iM&&#
3S%&$ jü* 4nr&*
&aatüür tB%&8«üLeg&db& a&rom IGh# ipr3w&t&«M& %K>&Eds ef
gpMs$3%(%* iWbo
f%xr l&t
c%f viübrmdslooi glidLog <&in&ry ia&g&t
eoa%poa%M&odULBg larltlaMCl a%w&4H& smdLl «dboiN» t&w& %%yr8#& ogwor***
t&on p&u o w ill not aaually he inveatlgat##*
A good
pro%lm&tlo& to the B##t Imnortaat a a ta ra l fregueael## o f
t&%&
i%#o pGK&oel&w&l BKM&ee cwf vll%rat3ü8a gww& he <*btadha»&
iby iMaduadbsg t&w& egpü&yaldw&t
or threemmams ayetema#
*Qr&t@@& to (ühapldMP tm#**
However* eoaaiderahle e rro r may he
Introdueed &a h&adllBg gome ape&lal oaaea* and the tahul&tloa
imothod o f G&rrylag out the frequency oaloul&tio'@ hoeome* d
daelrehle*
Ihe jhMK&B&agy tahul*tdk%i%a&tb&d la haaw^ltoxaa the thee*
r%*1&&eail
IShw&ls iG&ie iiaLtussaul -ESpGMgiagKBHBgr (%jr l&cxpi&loaa*
&3L iflbipatdlOKi <%9^p]MB3%BMG%a(l8 iso <& &(xow3jLtdLon (tf <*gp&3L313)i*&t:B* ttort*»
TBSHBKi ta%e 4&]Uaü&t»l4& f%*rew»a*
#*i%d t&aaa l%%eKPi;lj&
jpi'CBa t3&#
(OdT t&&«» tKkuBdTi;*
(*f thw@ CN*4&i]L]La1b3kBy& isw&ewee*#
%>%*&##:&(%& <%f tx)%*gp&ek iii; auQF OBd*
«iloiyg t&a#>
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(%
ww@to
tüsa* <)g&odl3LlaitdL<%OL <%f tab*» zawt#:»#»# (W& ggaak ladUB*» oik ibbwads ]po3j&i; i&ika
the eqeatlGB* o f torqw# &&& b* **$igp4%B Wa#
gbd&e th# egBdltiea tb&t tb*e#
i# a& torgw* a t tb»
o f tb * gb&ft# the ##&*&&&& i#w&
bo eolved fo r tba fregwmagy
<j , dbi#& la &nalw##& È& tb#
eaproaa&on o f torque*
Tbla w ill eoreogpond to oae o f tb#
BOtuaml frequeaole#*
The method o f oaloulatlon due to flolee# a ta rt# tb# e e l*
oualtlo& w ith & rough g&e#* &t the freguanay*
The
t&OB o f aJ fa r the fle e t t r ia l eaa be made from the ealeu#
tiom baaed on
3W&A&@&& two# or thre&4m&ma eyetem#
Aaegm* the ayetem ahewa ia Pig* I# ( #* L6 ) to be
vih r& tia# w ith the freqwenoy o f a ^ i *
If
w#r# a a&~
IbaawCl j%peqBB&n*gp çwp $&%& agratMom* ai f%*@# iribs%atdkx& 4&@u3UÊ cnaww»
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&edb t&w&
ads oew&b laaa# be tha* fogaa <wP
ftüLlÆMsa iBbedb t&w& awBoeOUergd&lcwi w rill Tbe
#&&6uyjb; jit
a
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1 3&adUhKB» i*<&* #
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^Ige 12 - Seven-îvlass System and
Its équivalent Two-Mass System.
"r+1
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Fig* 13 - Adjacent liasses in General System.
w
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ga«tiœ sf tte® «feaft
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g&KaWB 3Mgt*a&tkl#ak aaJLlei;# 1B&%
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jBgwaikdl t#bwB%i BSae ssBkuJLe
4SR%la1%
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iBe%pg*akoü%GLl ;?ljgjLdWLt%y <%f taawk SMpgpwrldPigB 4N94*1%&g)%t <%f
#&3%&
already knew#*
l!i ]K*lgS, 3L8 ( ip* !&aS
j9w*sRa%QdkBgg
«» 31
4aw%& la# jREMi3%Gl j&i40%% G&&& la&womr# «atBOw&tdlçMQi*
jlik jBkuajTt;
SBrwoiKljGg; IBkw* iBooptpa**
# *&%*' t%(kP(%uw» las js&kauPi; Ic^,; **GGF
:gy*G8m tàbeaw» t&sa* (&%i
fig
48%>i%ajLE%&&»
<%f Ibmr&iét; <>f $*kw&3*t Ikq&g awsdl
*ib<k,
:B%%3r Tbê* <saLl4%uülcL$%»c%*
I>3r
t&i& f&Ggaat
tb# GBplltwdm e&
be
t9aw*
<>f l&sdli&t jLoi
iHy&iB&GiKibratoBy torque a& 3^ 4#Bi
#Bd *0 on tbyeug&o&t tb# Whole eyatem*
F in a lly , arr&v&BG &t the la a t m&&8 1* , the y&b&atayy &#p*
que le expreeeed by
*
3b order to have the eyetem v l*
brating* i t la n#@eee&ry to apply a t
ly
* * #%ter&al to r*
go
qua#
Dut Wbaa
happen# to be & natural freq##B#y*
tWL# remainder torq#* *9#I& besom* aero and no eater&ai
torque vou&d be required fo r the deeoribed vib ratio n *
I t l8 neoeaaary to aeeume a valu* o f
#o th a t
the remainder torque beeome# aero; he&ee* the magnitude an!
eign o f the remainder torque might be taken a# & refereno#
fo r Ohooalng
in the eut and tryiproee###
o f the remainder torque
i * ehown In Fig*
As^bbt
9^%% verau# the natural frequeaey
( P# #1
%b* behavior o f the
remainder torque 1# u#ed a# a guide in eatim ating the ear*
root value o f
<0 fg# the eubaequeot t r ia l*
ObaerviBg the diagram* When
must be alao aero#
ia taken aero#
Belo* the f lr a t natural fregueney
f@%t
la poaltivo# between the f ir a t and the aoGOBd frequeQ&lea
i t la negative* and ao on*
a t adjoining
Bbe Interoeptlona o f the eurve
natural frequen&iea *111 beaom# fa r apart a#
I t @08# to higher degree mode#*
In order to lllu a tra te the eourae o f o&leulatlon in
building up the frequeney tab le#, nomerieal example# d ie*
ouaaed in Wilaon*# book are reproduged in the follow ing*
3k*e I%#n IB&rtK%&#ar Iboc&cs *^8e@&wKnidH&l TNlbr*Ltlo%#
51
ext O
Natural
Frequency
Fig, ll|. - Behavior of The Remainder Torque,
_Gen,
Fngine
I
a)
27
165
27
27
165
27
165
27
32
l(S5
b)
Fig, l5 - Direct-Coupled D.G, Gen, and Its Equivalent Sys,
3,3
i W tlsw »* W #
D, c, Seawatlag Set#
page Si, Voi, I }
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wtmAl Imotmllatlom 1@ whom
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O baraeterletloo o f %be ^bdel System#*** In order to
have the performance o f the model gyatem e im lla r to th at o f
tho proto*type* I t 1& neoeae&ry to determine the condition*
under which the model eyetam re ta in * the aame dynamlo and
e la s tic eh arao terietic* o f the orl^ln & l ayetem*
$he baaic equation expreea&Bg the eem&nti&l <%f a3%&r*
monio torelonal vib ratio n la repreeented by equation
&
•
1 / 2-n-y k% / I
68
where
I
*
m&aar moment o f In e rtia o f the vibr&tl&g
body*
#
tGrala&&l
?rom equation (9 )*
«
rig id ity o f tba ayatam.
la given l&y
J & / Z
Bet the edb&er&pte p $#%&
as
gondltlon# on the
protowtype &nd model* reapeatlv&ly#3be i&WWLo <%f 10%* jhw*»
quenelAB eaa be obt&ine& a# fo lio # *;
^
tl*2)
Por e clld olronl&r abaft*
iTdA
J
m -----------------
32
and #&&& both of the dbafta are mode o f &gme m aterial#*
tb la equation boeomea;
( fp / & )
s %
/% )^ ( 4 //p )
/Ip )
%bl& abowa th at the ra tio between the freguenaie# o f t*o
alm lla r ayateme depe&da up&m the relatio n # between tbe;0by*
e le a l dtmeaalona o f the two arrangement#*
I f tbe d é fin it#
r& tle# era aot up between the oêrreaponüng item# o f tb# two
ayatem# reapeetlvely, the fraqweBGl#* # f #b* proto~typ$ %*&
69
b# predlotçd from th# result# q f the model tee&m*
^#3
Jerque Control In rorned V ib ratio n #*** I f an applied
torque
gin * ) t . la acting on the aya&em * tb#
foroed vlb retlaaa o f the applied frequa&ey
It* prodm##*
%be eaar&et&r&atiea o f the f&reed vlbr&tlG& depends igpoa #&*
aroporty o f
&)
ap^llod torquu*
Ppcpmty 3f
#la# D riving TOrque*
gb# toraiwB&l vibration# Im the arankabaft o f a roolproeat*
ILn,; iBn&G&B#. aa%* ea&sltM*! tgr t&w» 233BF4&8lj5&rBd&tiaw& 3b&
IjsKS
jL# <i%üoa;ldb&ZH8Ml #& ai <:cxc&>l:]akt%&<%ai <&f3P(M8l& ladT
IWhue iLGw&Bf&jlgi {)3* ibfie
part# ecnKl t&adk ipeedlCMajla iy%K%d&a*&dl<%BL.
din (33<Ij&a%db8%' (;,&* vysHowszaajp*,
%&ce3&yuu8i:&j3%%
dtpiiGwadlc; latpwagr <038 üüt#*
cTwysra l%jw» garaeaSs a&i&TI; -toiq&ua (%@83*&l#%IKIbQ6» <%j8
taaj&guD <K3B%p\3îï€9%t;o <xf cllje:\).?P9%ib
tü&<% tü'itglio <3%
%
@
3^e(:3^p%p<>G%&1bi33gs %8e&aw»oe, 3b3d*x*tt@L Ikc/Agui* dkuw*
<3c%BWüa>crbjü3(:«'%%3(l f%i%i 12%* .gpaat
]i)
is&aaKtSjFi, j&agôp*»
1%e%p<guw9%k
15k)%%g%%e '
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%
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> 1b%
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ISasKZS) iPSNSMsjbMW*
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pljledk #%:gp%2Gw* (%(» {)(%Ek9dld&Boe%k%tl/» TFâü&3L9Ltül*%Ei <9&i#epqad»$&@8pdLaktdl4*ai 4a%
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k
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(I
laagElKWf# **& <**a*BqpC&dk <ad8
tabw* 8%%%* %%%M9M»8Muwp**f aj8**%*BdL*t #*%%& # # ]p**aMa3L1%**%$& j8QW%WN* #ap*» T&Sbùdb*
ta»a Aga tm t BS&ê (%*q%%dk&»aaag;I** aa# 8&woMK& âl%&ZP&jB#; 3W3 ( a#**»
]B\, la*, (ScMQüadkB^isi l)GW3&E* **Ikea*ljBa <»&* laSkgft
t%&(8k iSeysjliwBW**# C%]w%pdb4aB» 32
:%k%$w*$iQ*&3L i&8gdi%BW*"»
iEkw* <%*dL9&a§E 1b*%m%wwk <%& tüaw*
i&xMBwa&E iBKiadgi; j&j* %a*&db» wqp %%f igbw» pq&gnu&tkeaai: jPcwyw* 4a@c%d*t%*a%gs ladk
jaagr jLEwaiaaatt, ILii IBkwa agysaSkek»
]DEi #%%%ak&3F2K&n@
; IB&w» {%%dli#j8#g ibKKÿhgsaak <)dT 4%
%
%(ezagglsa*** t9bw& $%&*»
iüaZL :PN9<%îj)ï!GW3aktKÎjo@; saakaua aa^pg^g* * iKhLi<)&i ]âqp(%a*&<w8w» IGaw* |jad%p4kaL*i
t%)3*qp*8 iQd;t%Ia%(g <%
%
% GBwe» txEqsiiïE 4*&wadP1% ila;
laws t&i*» leoBBi <*f IBbwe
iBEkaw&G*; <3d8 G&ie ipdL#rl%B% aa;4»#a&)3ir #*%*& <t i>awft <Kf tübw» SMoaaaaGHBl&jkB***
iPcdl.
93aa» igWLiP3.adl()%& <%*»
lOdT j&c%%iEW9wod;3jn*3«'%*3K3 laoi;* jUki* ip*»*»
3Kl2)39CHBwi1%%jG|g ewoKl :e<)1%gK&3k8ig ixwfba* «w*%%law» ]p8P*k@Ktdl<%*Ç&]l3r i&d&CHsaap»
jpljlaüMkdl Tbgr ip&ato&ng; IB&we secHi tkOQp^lsBBüïl&aL&SLar <9&i 1%*#G i#<%*dLakai*
!Z5%@ 3L%%eapi%IL& twoüpqpa# awaai Iw»
jPsposa t&aw» ipdl**tx%% jftnwBW* d&%#k
i%& tü&MB 3j3aM"tdL& *&(%tjLoa <%f IK&w» ifSosjLSKPt&akaiKSjBg; lüKW&a* TbgT isailtül'»
ipjüÿiaag t&kG
aübjajrtu*
sabL#
(%0R&9W&a*4* Tbcxdk*
5*
izKaB&eadb
4d&HGR*i& taie» j&asjUB» (%f IW&w* tpxMiaa&c
jf<%p tabw» ljo4*%ytaL$k
<3huar)i&ear
Se# Bibliography Im tba back o f the pepw*
jl* |%l3p<*a jlit
71
(xas Pro s a tire
R e s u lta n t F o rc e
I n e r t i a F o rc e
120°
0°
2i).0°
360°
1^.80°
600°
720*
F ig * 18 - R e s u lt a n t Gas and I n e r t i a F o rc e s o f
O n e -C y lin d e r» F o u r-C y c le » S in g le - A c t in g E n g in e*
360*
One
Two C y l
F ig *
19 -
I n e r t i a To rq ue C urves f o r 1» 2
, 3 , I4. C y l*
78
1
%
• — «rro
#mp#
(%
* gPg
* 3F| s W #
1% *
# * aemak an#!#
# e a a j& l& r v e lo c ity o f the araak Wb&ft *
8B&
a#e e#B&t*&ts*
a»0 g*pre#aea &» fwaetloaa o f
q #
Rj/&
%&*** a@a*%ma$#
# W%& amWÉk»
o f waakwp&aiu# to lea&th o f tb# @oBa&otbge*&&&,
!Rw%r%mgr
%%& <&ctv<)%3BKl%%aH3l jCï'CPi @
L lejfwwaar odp i#9w* dGrtssBadltw* (xlT iB&wit (8%%a%i&e aaWksüap
(KB&jRBi lOdP sKBi (azii^Lno#
!3&*e Ijow&aftdlai twoecgQa» <aaa*%F(&a j%BRp #& 3e4*<&#/»
jpseocwajbjlisg 4a%%8ÿl%%a& i*dLt8i 3. ,» 3%,* j* j* && (sgrlJ&BdbMP*» laapc* aaasyaga jkck
iPaiaB* 3.5» ( Sk# TTl ) ,
^ISbd) gpaa# p:Ey&g**B83P%* tKsssgguw» 318 t%a*wu*Ol]kaF j»iB%&ddL4&dt Tbgr ai tk*K%*aN»«*
a la gaalyeia*
F&g* $& { p# 7 3 ) dhow# the g#8 torg## o f
008 gylloaor o f & fouz*ayalo Dl##oi eogloe ##& it # f l* # t
throe hirmoolo eompoBootB ( aao D#& Hartog*# hook )#
%h#
Irre & h la rlty o f the torqoe throwghoy# the oyole la evldaat#
jod the avoraco torque delivered hy the oyllader ie only &
# ml l ;Eyp%&@Ptjlc%Bi
tacw) 3k&jpdL%%g;
G&io aBKaasIjgaaaa tK>%*epjw& BrijLcti <&gw3U3*@f <3%%%%l3i(g
]Et 3La* iakl#M& s%
<&@
ü%tawajb t&3w8 tasjp*»#» SawsaaawaaajLa
OuuMfswBt <%c&db»d tKsgertkier agjbma#) ai %"CRiagbi **a%gwp<)ic2j3Bkt%#wà%% <3d* igaat @a&*
tawaal, <giieif*wk* tmutt awaaagr zaw&ape %wBUf9BK%Qdla oàaBgpüàsâaa&is** 4*3*8 3peq%*jl%#d&
ibo srqgpKreawBR&lb tïie ibcxEtgu** lO&EXMre laa (%lf%a;e dlelba&jLlH#
iltt jL#k i@Ki3;y'
ikci iZbke j;<Ma3P*"aqF4S3L«» laiygZlss*» IBbweKt ISkwBrs* 31** 3Sd*]üES"<%3%à**ap 33a&am:;9&&&d8w*;
73
F ir in g
In t a k e
C om pression
F u ll- L o a d
H a lf - L o a d
Id lin g
A v e ra g e
360'
To rq u e
720 '
— o rd e r
1 o rd e r
1— o r d e r
2 r e v o lu t i o n s
F ig * 20 - The Gas Torque o f o n e -o y lim d e r o f a F o u r C y c le D ie s e l E n g in e and i t s F i r s t T h ree H arm onic Components<
Td&llat #0# m t*&*oydle# mingle * aat&ag eng&na# übawe tba
working eye&e la p#rl&#le * ltb #8* revolution e f tb# emwdk
abaft# tbere are a# harmonie oomponent# of the h&lf*or##*#
3ba m&thematloal theory dhowa that any perlodlo ourv# oan
b* apllt gp Into a aarle# of almpl# harmOBlo 08rve&$
Bb*
torque eure* o&a therefore b* repre#*mt#& by a oonataBt term
aa& a aerte# of harmo8le#&ly varyla# term»*
Zhe general
eK&re&alon of the Fourier aerie» take# the form#*
f( # )
*#*%} + 4 ^ (d b i# + *^ aim 2# + *$ #&& 3# * * * *
+ b% 00# # * b# 60# 2# + b^ ooa 3# # * * *
%here a#
la the oOBateBt mean torque* and &% # #2 # * * *
and &1 * &2 *
**# eonatenta lndl&*&lB& the amplitude#
<%f ^a%<» lysaarlosM» jbu&rBxoGsdLo iGxsagpHOqo&xBdba**, «&ijL<aa isaaai %>#wgb8db<k%s%dL%*#wai
jEypcKKk *%n eBM&3.;p!9jLaf <&2T t&i** txaopquwa owaaeiMak#
][][)
IwaapBacMOdlo jla&sLIarsKSwe <%f tBgKays*ki%tdLs&l
jToz» .ïlüygOL#*
(?3r%jL%&gb8a* <}jp 35i#k jSbigEln**
%agtt9bodL <%É* :li%*pea#1%ijsaktKl<>%&
])#%cg34*3T&dL*&»
jüGwg: t%)3r(%wws ]bu&*& ]b<*<*n <&gr#q)]Ucg%4»cl tsgr #C* 3%,
o fioot (%f jLzBGrtAla
4%%ia
3L%i %*Kil<8&k iB%*e
<}a& tK»%*qKW» j&a* 4k#k&a&%& 3L%ttx>
(w)ip%*eH&t:3Joy% IB&ie l&eoPBacMajLe <*cw9dr*^lj%#^B8*1&8 cdtitsLinaNl
edla# là** kÈ&g* i&ew* %%r&&aHi3P%* <3%*pir4» jBüLowsw»*
tKgr
4K*i **i%eû%3P**
72
In
(aawspdb*** (S** TRgüL 3[# lab*» jPt9%GBdL#*%» #M#9PdLaw*
at#» iBÊWagpeaadülbaai
(aagpqn* jLa T%%dltAM*& *%*;
9f i*»
or
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$1
$B <)ipdb3g» aoKtaJx**»,
#
3* 483M8Bo&e jaaaggle# #*_ja%%p:ljL1%w%34k <)*? 1B%%& lodNBi <%*€&#» 3P%&aB%]Li%aa3t% iaaoesac»*
III# 40H3B%2M3;s*Bi1& (OdT GwKEygGBRktaLaCl SKfSf<xei&,
(C)(
** idkuaaw* i&rkgSL*»* *BOK%
J&%a* 13%^* (KBg&]Ll1b%&dk*s; 43I ' iBt#
lOLlBkt <>;Makwr )**K**acwQjL<* isaes**
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j&3%c& :Li; <5#n Ik# (dkwORwn IGgr 'pOGlboz*
GBaett
a
(SX'ak *f Z3%
%/f
95&& aagwazi ib4%rw3<Mai>l.ja]l (adf'osMGgp
equatlcn #
% b %a
%
#
2 ac a X B
awaaa Ibe (%«Ct4âüdL8Lt&&dl jf*# ** ik&w»
of platan a&ewb
&
# ta t& l #%eok&* fdatb
B
a* mp*ak dh&ft rpm*
a
e aaadbmr a f iwarklB# ayal## par ad&wte*
B
* B&adk &*&&&#* foot#
liGRBae, jCtKE» jftMULptm^RgneCtak, i*3Jc%s]L«h*jaw&t;lj33; «Q9w%&oa@i** iw&%aBP%*
%
%1* Ê*,/ S& sucwl IL #*
%
«
% / 2 TT
Wov #eabl»#m ettag o r feso-<^el®
«bar®
H« M,
%
»
&
%
«
» a /- n -
3&W* iWBpr&Gtloal%%p1#%*
1* than m&d# ta tb*
a f the jba&ptlm am
harma&la aogpaaent#
* 1%r
& dyBamla etudy a f the vmr&as# inovlag ipapt# ragpeetlve^y*
I t jb&* b*#& Dot*a th a t tb * iB é p ti* &*a aomparatlvely anail
Ita a w ia a ffa e t b#&
:b%&4##üMüükl1# t&m ia t* %n&# and 3rd ar&MMb
A
tb# raaultm ot haMmaBlg aompaBaBta a f taagontlmi e ffo rt #%?*#
77
fo r 08# eyllndêp 1# abown la Blleaa*# book# wbldb la ôoâ"
p lie d from pr& etleal #*&& rel& tlag to the variosa typ## o f
eng&neg* and I t may be waod a# a good approximation im a&#&#
Tdhere & epeelal h&rmonio analyala ha# not been made*
III)
GGüblB&tion of Harmonic# fo r h b ltl*G *llB d #r Shrine*,
In & m altl-O yllnder engine the torga# exerted on the drank»
#h&ft a t e&dh eyllader imay be ##pre#eat#d by a éompoalto to r*
quo curve a# thonn prevlonaly In Fig* 13 and 20 * whloh eaa
be s p lit up in to It# harmonie eompononta reapeetivoly*
In
order to obt In the reault&nt h&rmoBlé I t beeomea necemeary
to eonblné the jroup* o f harmonie# o f equal order but In d if­
feren t ph&ae*
Thla can he don# e ith e r by adding together
&# vaetora the reau ltaat harmonie component# o f varlou# cy­
lin d e r* or# by adding a ll the #ln# component# and the eo#ln*
component# reapeotlvely* and then eaWbinlng tb# two resul­
tant#*
The ybaae re la tio n b'twoen v&riou# torque harmonie a t
reapeotlve cylinder# *111 depend on the type# o f engine# and
the fir in g order o f the engine*
According to Oouain*# aba­
tement* a convenient method o f analysing the torque harmonio
o f e o ita in type# o f eajinoa i * to regard the engine a# eona latln g o f a number of t*o *o ylin d er lenlt# #o th a t ;for eadh
ipajj* o f 4%yiia%ler# i*# gpyt g%8k eagKloadUan fVn* e$wd% r*MPOlBdKlo&
<%P the er#Kd( a&wwft*
I t 31# alaw» #dhdL#&b]k& to <ira* IBbe
dbjUdh 9WM» 113aw»tr#d%*a &%k l&llaKKi*# tKwok#
3&)
SB&rqg# <3o%d%xXl asWl :DrlTdk%5 AasM*B$#g*%Q# i%KP
I t %%&& bew&a a&KBBB t&w&t tba&
SysMbwa#
o f iBb# (gnsll# lâ&p&ajdkoB cdE
borgu# o& #& oaclllatlm g
earn be found th e o re tic a lly
from tb# harmon&e analy#!# o f tb# torgg# ewve#
jRowever*
el&ber&t# @#l#ulatio& *a& oombeream# work on analytic and
graphic method can not avoided*
I t i# * therefore* o f great
In to ro et to Inveetlget# % proper way o f oontrolll&g the appdUkxl torque OKtsëWWüi ieyateok
t&eu0bt#%wMM& ]L&d to the IdkMicdrtiaing & oaaM
d rive eyatem to put tbo torque curve in to the model system*
d&noo the e ffe c t o f the eimultanaou# application o f a num­
ber o f external torque# to & torsional vib ratin g aystom i *
equal to the sum Of the effect# o f the various torques ap­
p lie d in d ivid u ally* the p rinciple o f lin e a r superposition
eon be applied*
P ig, 13 shows the resu ltan t ta n g e n ti*!
e ffo rt acting on the crank shaft being made up o f the in e rtia
force and the gas preaeure#
The disturbing torque may be
introduced in to the model system by usine two groups o f camdriving; one 1# made to give the in e rtia torque and the other
i# made to exert the ga# pressure*
Othcrwi##* both the in e r­
tia fo»cc and the gas pressure o f each cylinder may be put
;#&& single cam-driving medhanlam*
Per m u lti-cylin d er en­
gine model aystaa* due regard should be given to t^e phase
W W w ##
# w .ft'ad&s oȉ9T
te te te m m
te# vmelmtim ot tnwik te a ft #PMmge*
S® «©aftjssl tea âtttetfeias teg#m$ te® meter #teteg «#«
hm
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80
GCLKKZBGRXKia#
:K83BGr 2BB8T5a(
!>#1 B*a%wpg (WP Bkkb&I
:Et %ww& %*w%& awüitidGMWl t&w%&
tb * o s c illa tin g system o f an aetaml In a ta lla tlo n earn b# re­
placed by on equivalent ayetom* oonaletlng o f a eerie * o f
m&eeea eonnaoted by eeetlon* o f ebeftln #, wbldb re ta in *
oloeely tba dynamlo and e la e tlo dbaraotGrletloB o f tbe o ri­
g in al arranjonent#
I f & model eyetem la oonatr&oted thldb
la geomatr&eally s im ila r to I t * and Id e n tic a l m aterial# are
uaed fo r oorreepondlng e la e tlo part»* tb e lr natural fr e quenole# w ill then b# almply related to eaob other*
I t la noted th a t* In the free torsional vib ratio n #y#*
tom* three fbBdamontal item» are o f gro&t importanae* namely*
the m aao-tnertia* the torBlonal rig id ity o f the abaft and
the dynamic arrangement o f them*
Therefore* i f the model
ayate# 1* to perform & & tl8f& otorlly In the experlment&l work*
i t l8 evident th at a#*y and rapid ehange o f :m&»#-&narti* and
e f ootive abaft length 1» neeeaaary*
The oonatruetion o f
the model ayatam henee involve» a oomblnatlon o f the theo­
re tic a l oonaldoration and the p ra e tla a l work*
*>*2 CkB&atBN&etjkxn
1&&# %B&*# laoawmt
1%%*
2
SBdkla 31# «Mfalaw&teii f%%B& %
2 rg; * <%r <K%3V<Ri&e%d%ly (SK-icaawMi »a#
T*
as *
o f i&ysHüklcmu* %
%
%# 3L* & jfuzwyblOBt
o f lin e a r dim#8#&#B# and can b@ ooaeldered *a proportional
to tb# diataB## from tb# axis of ra ta tio n to tbo loeat&oa
o f ama@*
H#n## tb# m & *»-in#rtia o*a b# put uad## OOBtrol
o f & oonatant weight by moving i t toward of away from tb#
##&* o f tb# dbaft#
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*%&& @dttaa&%#d 4&& *B& #&%& t&dkdb j&# awwÊ# <%f 1a*9
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3&%*k
moviag y&88* o f the weight* o& veaioua length* o f dha8n#&»
888* @88 eetim&t#a a t tb# cantor o f the wel&bt to the can*
to r o f the dhaft&
Ô& 6* lo a
# # %i/% 2*
to
8 3 /8 *
On p* long dhaanoi#*#**
r * 1 %/38*
to
3 %/8*
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r # i i/3 8 *
to
6 %/&*
au
c e n te r h o le
d r i l l e d f o r l / k ”rt -2 0 screw
( f u l l s c a le
P ig . 22 -
)
D is k W e i # i t s .
f a s t e n in g b o l t
and n u t
6
P ig *
23 -
o h a n n e l-a rm
lÆ a s s -In e r tîa A ssem bly o f Model System .
j&a3U&otl<8i odP jBbadPk#*"** S&w» to]n*lo@üül *dL;gldjJ%r o f #&wüft
%&k # :&8 <H%ls&üL&t4M& f&<8B t&w& ft%sa8jU& (9)# #%kl i t I#
&&k t&K) ]pa%MMc%w& a&wsptwBP* i%> %w* ]p%<n%o*4%&o%ϟL t#
d ,/ / #
Izi (BPdkBP tx> gajja saw#* dba aww&BQüdkQg <%f t&wa gw&pfossaaBKW» o f Bb#
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of
8BK1I I
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SCbo <&p*]Ll %%%& oqr $&w*
48%%M* %dbp*
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BB&tKM* azwS la radaie# :lo%%s aM&oak ]L*By2#hk
%B&8# <&f ta%& BK>da]l
SkarfyUBloaab adstfSS»
<xf %M&apdb%8# #*pe %%o<#N*aeB%r ##> t&w%&
drlidLnf 18%%%R%0b 4&*m%@&@ru&&&aBa ftgp aad&eyswül txxpqiw»
tdloa jLf& ]pd*3s%dla*3K&Tb]Let»,
3E&W
E* %awi8a^*dL3W88p4sdla a&apo 4o]L*sB%M*dl <%;& tSaw* e&w&ft i&e* j8üaeM8& jbck
ZPyLgp* i&J)*
SZkbG <;(xr%ta?0i]L
<3wf tGsw» <dbwaa3rkail4*a*%g;& laa*#! 43a*3»ljL#"
odl ladLiBb j& agawkiLIL laKtlksw* Iso %;<%ww8nBBat <)%i tiaa* a&iaft aft#» ibSLapadb a%jk*
With tb la mrraa ement tbe a ffeo tlve lon&tba o f aeotloa# o f
shaft 8#o o&aily db#B%&*&le*
IB the f lr a t aotwgp* *
fo o t la loagtb #a# used*
l/lô *
*&**% wire o f about 6
I t dbould be a*ted th at tb le
round rod 1* fa ir ly uniform tbrougbout It# #bol* le&gtb,
3b# shaft o f the model ayatom may b# mad# o f two rod# o f dlf«
foro&t diameter# by joining together w ith rig id eonaegtl&a
to give the deaired ra ria tlo a o f th# toralon&l rlg ld ltl# # o f
varloua Beotlon# o f tb# ahaft*
5»^
Supporting o f 3b@ Madel Syatem#**- Itl& aa already Tboea
86
ebowa th at f&#@
are *a*out*d vltbaB t any external
&&6&&la8^torgw# aating on the ay&tam*
3h@refGr#, tb# p r l*
38#ry point o f aqpportlng the iM&del ey&tem 1# to latro d o **
I l t t I * or *e goaatealBt at all && the j%yeb#mjnMx&<ngF4Bé*
to m a l Bowree* mo th a t It# natural fregaenole# w ill be tb#
#@8# a* th a t of a fre e noasopad vib ratin g *y#tem*
3bl# baale Idea Im pll## tb&t theiBoàol ayataa jdhmiW
e itb o r be eypported on a very fre e upper bearing or an##
a eery t&im long wire*
3b# e rlte rio n o f the
la tte r method lie # in the fa s t th at the toraïonal r ig ld l*
ty o f the th in long w ire le a a a ll oompared with th at o f the
abaft o f the model eyetem*
I t 1# then aeewmed th at tb#
model eyetem ie In e ffe o t & fre # v ib ratin g ay&tem#
jl)
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la #lg *
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( p* 33 )* àbe*# tba aeaetruatl## o f the *wgp#&*
8lOB amaembly,
Mbte to Pig,
:&j
3bw» 8pdknd3j& la* iaedb» odf
:P8w%%& twKP cüf t&w» a&WKp#
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;2) Ji aBBalJl ipïays ojP t&w» sijB* t%> gjbpe 48%ug jf lt ibo ta&e %w)l#
dbdlilawl <83 t&w» agdkadüU* iat i&awKi t%> 4&K8&# tgp t&%* sdüp* idbie&k
jla twqo&BMi <81 t&M8 @%dLBd3U@ tgr ]paw&@l%g& tbaHeuggi t&w» hole #ük t%w#
lowSMr 8ZW& ,
À 1F*notdb <l8 <%it <«& t&%& awwefaww» oj» tha ]p3&yi
!Eb# IBbytü&t
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Ik&a&w&d adk t&w* tcg» o f IKbe %@od&dl agnateek *t*8a&.
88
S p in d le & T h ru s t B e a rin g Assem bly
Top fro m e o f
Model s ta n d
S p in d le
T h ru s t B e a rin g
©
k iA " -2 0
ta p p e d h o le s
on 1 7/ 8 "
c ir c le
fiin
l/If ." ro u n d p lu g
w it h V ^n o tch
5^^
Vh
( h a l f s c a le
F ig #
)
Q-
I
Ho# 7I4- d r i l l f o r
s u s p e n s io n w ir e
( h a l f s c a le
2l|. - S u sp en sio n U n it o f M odel System#
39
0}
The model #y8tem aboulé not awing to and fro In tbo air,
and tho abaft nuat be guidod to ollslnato lateral vibration,
'OoaLO, of b
eond
i it la nocoaaarg to uao aomo boar*
ings to keep sag oh&f^ In placo *
Tbooo boarin s should
bring no frictional ro&lat&ncc to the shaft*
apaelnjs bocwucn tÊio maoa-"l
Since the
may hcve to be oh&njod*
and the shaft might be replaced for different aot~up. It
Implioa that t'.o bocringo %mas D€ easily adjustable and
quickly removable*
Split notches milled on t^o sliding
plates can make a slip-in combination for thla purposo*
L the bearing supports can bo
ovod. alon: the upr
tao stand or removed acoa&laniy.
vj of
Pig* 2$ shows the con­
struction of the bearing sup orts and they are mounted cross­
ing the dl&gonalD on the stand#
© 4—
-
m
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trC
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;>u,) orta.
1j
1
jjL
2Sl»
% ï/S * # *p# !&##& te
m
bol
<m tbe
bole# are al## t@a&ed arouad tbe #«#tral # l# t fo r
a)
A V*notdb
% &He4at 08# en*
0#B#tr&Gt&#& # f ^b#
tiom
A b a il
fo r #mm#8#l#8«
mat fo r
b]
along
#0
r point
91
%ba SKWBWKW&aaof
ta%e
#&#%#& 1* fla#& gp @&
Amm# md tw W # rl% im ppo#*
pip&ag trea&a*
W rnmW <m # &
Tb* #tr&otu%# probably ibma
to t&msRda*
%&#&&## or ##m&31*Aio& o f the Ataaâ
&m orld ep tly ua&**&r#&I##
3b Plgb 86 ( p# 9& )* tbe #tr&o»
to r# o f %&# model eye##* #$*&& &# eba*#*
Bote to Fig# 86%*
1)
gba f*#B#e are made o f
8* x 3* x 3/16* ateel eagle*#
%b#y are beet to Wbap# *a& welded a t tb# joiate#
Tbe
era#* member* are meed fo r atlffeB lB # *&& fo r tbe eoapea*
adamof tb# model ayatem oa tbe top pleee#
are braeed o& the #*&1 by le g b o lt**
Botb:freme*
Wbodea bleak# are ##t
up fo r etraigbtenla# iwp tbe *$#&&#
&j
Ibe atmad baa e lx pomt* wbldb are made o f 3 /k * bl&tk
a te el pipe*#
g&tbrea&ed tea# ar# ##*& fo r tbe driving
platform # aad the adjoatabl# @ro#**meWb#r* #o tbeyiaaylb*
moved along tbe upright*#
%&# platform * o@n be aeogred
&a plaee by aet aerew# i& eo llar# Ibramad to e&diiMOB&Ugs
3)
fb * #eldlBg»n*ok fl&agea are #*#& aa& braeed a t e&eb
end o f the poet#*
la jf&oadUky
The eomplete etreetar# o f th i* etand
afN&ar %x>ltjbq& tkmma l&ie jnuKaapH* to ibot&i
-frame» <xa #&%» t%%> aaaS bottoBb
cZie cv&tuwdl adkB* cdT t&w» etam&otsure ôd» tba» îBodkül arrête**
*t8w%& jü* aÊKMsa ab% Bik&te IL ( 3&# 9C> )#
92
w a lls
2 X )
-j. wooden b lo c k
c ro s s
member '
m o to r d r iv e
p la t f o r m
flo o r
%
flo o r
Pig* 26 - Structure of îvîodel System Stand.
93
B la to
1 “ i> t v u 0 v \iT B o f Uodol Systom Stand,
Motop W lw A aartilar*—— 2 » t s s m m m m % qS «tes* «Warn
%6
is %M@a
# w a ®3»fe?ol,
ifSS
^
iê m «£ p%«#iaia@ & w % ^ vm>m #
m cmles* to a% m # *m # o moto# apwd o f
& l«gr a iw ft aosd a
wed*
p o ll# «TO
In %g* 27# #m steateSi Shows # e mshmmtlo a$wm#**
aajst o f ti» drivlmg syst«a»
ttjs f t # m *
# # i #@ #m@msiow itoow ta
Ml# œ raiîatol* @p@@d rmtm «W %» estlamWÉ # *
PKsstm toly*
A)
low %BOd fe s ta H a tio a .
H o tO P
HK!
#
TfZ$
Hetofcioa %%ttor=thp(w# Vmri#lo-'%e@d«Rpl?#
ftiiissr
# a./ a*(%
R oâ«ctii.a Hafilo #w o u #i S to p -P a tt^ s
#
1 / 3,75
MaiiitiB Spooâ at Casa % a f t
1?2S
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2 ,6 5 X 8,75
B> E l#
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1 7 2 5 x 2 ,6 5 3: 3,75
âetttalty #@ s lip oa«ild mot mwotawi im
.
# ,0 0 0
V -W lt # t# s ,
■also tba spO'M m tio w ill a # # W c lo sed %#oa # e mWo
9$
c a m -s h a ft, 1/ 2 " d l a
U "
X 1/ 2 " V - b e l t
2 " ~ 5 " O .D .
lt-- 8te p V - b e l t p u l l e y
2 8 " X 1/ 2 " V - b e l t
39 " X 1/ 2 " V - b e l t
^ 7 " O .D .
V"#belt p u l l e y
V a r ia b le * * s p e e d -d r lv e p u l l e y
{ speed r a t i o o f tr a n s m is s io n 7 : 1
M o to r
(
lA HP, 17 25 RPM )
P'igp 27 " M o to r D r iv e A rran g e m e n t
Siiowing Iiow-Spe©d P o s it io n *
)
96
§
•P
CO
>
î!
A
h
0
P
1
OJ
<D
P
csS
H
Pk
# # plW k
of
W
A
iW #m ##@4 m % # #
f3motlo&3.3y
#gr
60
la M ttla load w WW
#
3S#000
henee#
#m ao lw tlo n o f #%# a im o f #mf%# Wmrlmg# W it md
loy eta# W a w t takm # e atrsmcth of m aW rlaia Imto am»»
al4er#M^(m#
a a y w # # # W i#
m 4 fo r eommnlmee o f Im W lia tlw *
W p e rw m i
aatuel ploturo
o f OrWLog #y#W% la aW m la M #t0 2 ( p# 96 )#
ÿ*7
0am aad
&% mwrmlnlDg the a#»
twpoi fro q u ^ g ^ a o f tbe model i^naWm# a drive o f Wrmoalo
motlom mgr W a
@^W&#
llo d w atl^julmte # o oeG lH atloo o f tba
%ea tW w p lle d
oolnolde# laltb %o
n&tmmi fW#e%x>3r o f # # model ayatm% % pWaommoa o f
rommmw W ill W oteorved la tbé perfo%mmoe o f # e modal*
Bw dnv# fo r $W model ^ te m m y W omrrled oot ty
# o erefu lly # a lg m d mm eWLOb prodoma a almg>io W rm nlo
motion*
Om# m e t W token to avoid # e poaaltle lo te r*
fOrmme to # e motion o f #%e mm W ilie trm m m lttlng # e drive
toem r^ # e model eyatem#
A)
Dmlgn Of Cam#
% # p re tlm o f mm dealgn in t&Kle oe#e w nela#* In fW tlr^
p8
Vmrlom
ü f tw
m $ t ooweapoWL to
oértWba m ^u lw pom lM ow of # e em#
& # q#a la aaqpeeW
^ ^Ivo tbe fe llm m r & W m W W
I)
oÿ
Motiom
I t 1$ im #r#tood th a t I f a point la W 9 l% in a o lro u lw
path# it# projection on % dlw w tor o f the o iro le w ill hm#
# ei$#lo hemonio
A hm^mmio motl<m dlagrm im
prodneed in th i#
1# Wiow in Fig# 28*
fs
c
bz
'&/
28
II)
uii3)ple Barmonlo Hotlon
Ib# O eoillating ^ ll e r Follower#
3h order to prwemt the oai^lesdty o f a erWWmd m ilder
zmohenim owing to the e ffe c t o f the m n rn lari^ o f the eon*^^
neotlng*rod# I t 1$ odvleeble to me# a e^dLng follow er to tran#'
m it pure a% ular aaotion#
On #ie other ha## tlm déviation
99
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T%y a long length o f Intoraedia*» ahaftl##* the aodel aya&em
m&^bt be too long to be able to handle by th is model ayatem
ataad*
Ih la lead* to the Idem o f replae&ag the model 0baf#
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%be e tiffa * * * o f
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o f the model ayatem#
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117
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r
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G e n e ra to r A rm a tu re Mass
Model System
-
Test
1.
120
kZ^ X 27 X 165
7*708
tJ
2Si>.iîi
itr- X
X u,uuj5H^a
x %“
313.51 X 10®
0,003252 X
%'
/ ^ may be
If fjn la xariod, the ooprftspoading raltiea of t
oalculateds-
ops
cpm
2
®
1 .0 0
60
1 ,0 0 0 0
7 .7 08
1.25
75
1,5625
4.933
_
Inehos
■p « 122 ope#
122^ X 27 X 165
,
“
313,51 X 10^ X 0,003252 X
65.05
'
Beep the a@m# 8*t-up as calculated In ( l ) ^ above*
%
2
in c h e s
66*0#
7+708
44933
(b)
1*000
8*%40
13+180
Generator Armature Mass and ëpaolne.
Generator Armature Mass*Ip
#
23#600 Ibs-in-sec#^
ops
cpa
1.000
2*906
174*3
3+630
60.0
218*0
3^ (
38*
119 ) ! •
1 » 15* lAaaml-mmm
t « 1" ' #l@ k # # »
4 • %/t” W # ôl:itea
2
^
«
3* lm% bol-fc* mad nwfes
0% W 3&
0,00228 ,
0.000003&28
♦ 0,00462
* 0 ,0 0 1 #
* 0.0m%'32l{.
0 *# 1 6 3 7 W
♦ 0,00936824
r§
jg
Sf^
Ch*8dWH&#%Wf a%M%8i3%g**»
3B& <%éa#Q» $# i&aüM* i8%è *w*a# j8#<as#tBKi*#& adbaHj&rllgr
t&w*
48%* :#%p#adLQg ae&tdb&. gWT 3B&&81F %MMb*#Mwa i@&# #&%*
(SliMk <gdL!aM&#%* )%pww%&zy& a%w& 4&w*
e ^&eaays %*&at 1%*
&W&*
Cl)
#8# tb#
a f vib#*&iaB#
#
<#%% /& * 38*#
* 7 # 7 08 3C-- ,» SbjLSS!»*
27
u im
epB
apa
l.W
1.25
60
76
■
—m
1,0000
1,5625
/a # 9,13^5"
X 32 *
^
i# 0»Vi3l62
313.51 m 10® X 9,1355
.
‘m
InaW *
m
i
##62
-
#
47.1312
.2
313+41 % 1
0.W3162 X
.
1*
1
È M
3# %
13.1'
y
3.630
»'tl
*
fa®
174.3
213*0
# P*
%&%
1*##*
0*062* *
apm # th@
6%'%#* ^
( P#- 18). )#
1*8 #p&atn% *
7*?08 » 0*06$ % %
#
9,136# - 0*068 % 8
#
9#'
123
suspension wire
(0*02^ dla# about 10'' long)
^ ^ 1
l/I'p" bolt and nut
l/L" thick disk
6” channel-^arm'
model shaft of 0.062" dla
gen.
3 " bolt and nut
l" thick disk ^
l5
channel*arm-
l/2" thick dis
FI ;> 38
Ilodel System
- Direct-coupled Generating Set.
.
fla to g. - Fodel System
6 - G y lln ü e r E n g in e D lr o c t-C o u n lo d to G e n e r a to r.
Ill)
%b# model ayatem eee&llm### wl%b * l l t t i * aeekla# mad teea*
bl&Rg &R $&# vewtieml plaa# «&#& t&* motor 1# &e&v&og*
torelOQal pead&iwa
A
]a*f%*gwaBgy 1*
4 * ABBd&er o f 2&et# t&a Wbol#
olBdlng the aweponalon # lr# ie potmtlng *b#& the vibr&tlon
the model la peogream&B#* however# i t la dlmlalah## Wbll#
the drlvlB # epeed 1» iBeroemea*
%h# ataod 1# ahakea too#
but I t la believed to give no ef#e#t o f r#a&a#ae**
fhe applied frequenelea are o&t&laea by meaaorlng the
roaalBg epeed o f the earn abaft*
8he& the maxlmm @%pll*
tud# of v ib ra tlo a o f the model ayatem la obaerved# the ap*
p lie d fregueaey la taken a t th at instant to give the natoràl
freqaenay o f the eorreapondlng mod* o f vib ratio n o f the
model eyatam*
(a j
#br onawnode v ib ra tio n ,
oounted fo r
10 eeoonda* or*
fg& #
(b)
33*# opm
For t*o*nod* vib ratio n *
counted fo r
9*7^ revolatiOB# iha# been
27*2 revolgtioa* Ihaa been
10 a&oond*; or
f+2
»
16#*0 spm
Wî
(a i
6oiva*4«w»
mS. 3«leu3.«fe»4 BmWwO,
o w m a # TlWàtÊom**
(W.,milm$ed %e«p9aey#
# 60 eyo
#w t
# gS.g #m
;»
Bm #
e— —
60
0#W
<» 2*5 #
Cbî ■Wo» WMWd@ vlbmmWlem*:»
O gtm laW l Wmmaam-t,
$ 1 # *3 @m
# #
# 1 # *0 #pm
H fflE » ©
m
—----- -— » 0fC^32
i? lt*3
ov &.3 #
i%7
rated &,T#0 BB# a# 138 rpm emgla* ea#»
neoted t# tba pro p eller throagb a long leagtb o f tr&n*&&#*
elon ehaft#
lb# egulvmieat eyetam 1# eh@w& l&3%ak 17*## P*aP do# Oba#*
te r
1)
3 *
3b# oalawlated frequeaolea are*#
Satagdt
lAsLb epm or 2*7#8 spa
Bad MBd#
1#0%1*O epm or 17*3# ep#
$etW8p o f 3b# Bbdel
1& order to elmülate tb# long leostb #eot&o& o f tbeipr»»
p e lle r abaft# two wire# o f d iffe re o t
diameter are aolder*
ed together to m@k# the model ebaft*
G*re ha# beaa taken
a t joaotloa to #Bewr# the torelom al rig id ity *
"(i&)
ijR flja*% <]%r3JLiuakKr laawwt #ki%d 2%>aiojLb%o*
:Ea IKkLlsk i&gLae,
## 3L6.TH?*
d^ #
Shew#
( d^ /d ^
0*06àg*
a ( 16*7$ / 0*062#
# k»nuz3 X i(#
( l)
Mae* aod üpaGlna# fo r #o,
3L *
1 , g*
^6*000 l&**inM&#e^8
6
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im#
m# m
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pg
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f —*H- - - - - - - - Il
lï
(a )
iïo .
F l g . 39
1 ,3 ,1 ;., 6
c y l.
(b )
No.
i
I
1
1
2 ,5
o y l.
d n g in e C y lin d e r lias s ^ îk>del System - T e s t
2
OL
Ô
I
j* 0.0625
F i g , i|.0 - é q u iv a le n t System o f P r o p e l le r w it h
r « 1.7 2
F i g . ij.1 IJodel System
1
9" c h a n n e l-a rm
2
l/I|."
2
1 l/I|"
P r o p e l le r lias s
•
Test
2.
t h i c k d is k s
b o lts
and n u ts
fo r m e aeomd m # - o f v lW a ti» #
.
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diameter o f the ab aft,
j%B*
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0*933?“ fo r Mo*
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P ig . 1l 2 - Model System
1
-
1
■
M a rin e I n s t a l l a t i o n
135
Plate $ - Model System
6- C y lin d e r E ng ine M a rin e
P r o p u ls io n I n s t a l l a t i o n .
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I t ha# alreaây Tb##a
###&#& la Chapter ^ how engineering problem# may be atadlad
by m&GB# o f the method o f model te a t*
In deelgnlng a model,
condition# maat be o a re fu lly determined In order to retain#
in every re#pe@tf the ehar&eterl&tle# o f the o rig in a l ayatam*
Fredlotlan 1# then made fo r the behavior o f the o rig in a l
ayatem from the perform&nGo o f the model*
Ihe model need in th la inveatig ating work la oonmtruet*
ed In geomotrioal a lm ila rlty to the proto*type* 1*0+, the
id ealieed or egwiv&lent aymtam o f the o rig in a l eyatam*
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Ih i# e&preaelo# ah#»» that both tb# m&ea 3Bom#Bt o f
and tbo epaolng b&tmeea ma&a#* a ffa o t the fregwanay o f tb *
vibratin g ayatam inveraoly && the aqpmr* root of the lio e w
diw aaion*
%)
BoB^Ualformity e f %&» 0&d@& ^b&ft*
I t l8 ahawA ia the above am reaalon th at the freguanoy v*#
rie a w ith the #@#are o f the abaft diameter While the leogtb
o f the 2&wü^i#^4#*%BW#2Km*#tof ia a rtla remain wnabaDged*
3ba model abaft i& aaawmed to b* o f oaiform eiae tbe8#0&e#t
it# Vbol# length*
I f the model abaft i& not n a ifo r# in
ol&e, tb# frequency may b# changed conaiderahly,
II)
gffo o tive Length o f #he 8#@tio& of Wbdel Shaft*
I t %R%& gaw&UBBwi t&y%t* 2b& 0w&tt3j%g
tba* aàck&ai aQnete&&# t&w;
abadft awatea#; the cldwgp# <&f t&wB Bü&ae#düB#3d&i& set eawdb 48%& (dp
IB# 2H»otdk*& tor an imaotait (KB&al ibo t&w* dWLem*M&ar
t&w& abaüft#
BkM*G9%%p# i t 1# IbeajLevqwi t&wwt t&w* cdSfecüüive SLexk^Wb cdP t%w*
@w»cti4w% cdP a&wwft BB%y ta» gaMwataop t&uw% t&w» «og&eclB&d vTüiwe (iae
t<> the i%BKM%pt#üüati4%e cüP tiw» tijgitoKW*# <%P iik t bartaewm t&w*
%aa3W&#iiKM*ti#t elaegp aaai t&w* a&w&ft*
3^%%a 1&w@ cQQprgwNRio&k i*besm&
4ab<nn», t&# ibM&gwwKtey <%f t&w» aKM&el sgratKBR 411 t&WKP*j%%P# tw*
lower*
A# & m atter o f f&ot* vh#n the epaeing 1# not ##t
igp very oloae# the e ffe c t on the frequency o f the model "*y»#
tarn duo to th i* uncertain condition m&at be neg lig ib ly
am&ll*
^hen the anaclng# bet*e#a the m&*8#iB*iti&8 are
fa ir ly am allf a# in the te e t o f a marine in a ta lla tlo B * the
4&KP0#
III)
th# Clagpiaa @ff#e$ imcy b#
Corroctiaa fo r #**# o f Shaft o f tb * Mb&el System*
Ibe abaft &# ageum*# to b# weljbtlaas#
I& @a#e a Il^ b t
ayatam la aet ep * ltb am&Il maa#*loert*a amâ long aaetlon#
o f ah âft, aa la tb * a*#a o f aooond te a t o f tba maria# &B#*
ta lla tlo n # oorraetloa fo r tb# maaa of abaft may b# taken
in to aooount by follow ing tbe ru i# d#aorib#& prevlooaly ia
Gbaptér 2 *
B)
DampiBj Bffaot#
Ib * model ayatem la aaawmad to vlbrat# &a jaaiæm&mgww&j&MW*
torelonal ayatem*
I f damping la introdwoed in to tb# :mod#l
ayatom from any aooro#, fo ria a ta n c # , tb * frla tlo n a l re#!#*
tane# ealatlng in tbe a&zportlag bearing## tb# natorai ;fr#*
gw&Boy *111 be radBood#
lag
3bla may be verled from tbe fo lio *»
l&wt
email damping or
1
gbere
& < #_ # % ItuL*
n&L
0^
f_ # damped natural freq&en@y
M
I
# maae moment o f In e rtia
#
e
tormlOBal rig id ity of tb# dbaft
# damping oo&ataAt Wbidb produoe* tb# damp*
jby; i&Em#&*1&&lA&]pr^portlon#l to tb * v l*
bra&loaal velo o lty
*2
#
o rltl(# & damplB#, tb@ valu* o f damping ooa#»
toad; W iloh 3KnMP*#%waa*#k i&& $&w* *g%w&ltaaH& ojP
t8M8**lidbaa 4a% frswk irl%8Nktloa i*it%kirl*4KBw*
dmplag
IhdüB a&wBPB t&u&t $&H& darngpod %%&twGMdl f%MW%#e%wgr &# iloasBr tbaaa
iWb* %HB&a8%M%& %w&tw3NCL fïNwaoaw&gy*
g&WM* odP 4&
A&#K»* t&w» r#aK%oaB%&* édU**
id ltb irl*<xM&$ dbaqpiay; ahoam* tba*
tWCfsw^b odP daBgplay2 <%% t&u& fymaqwww&egr raddLo *%t %q&@o%wKBawk
3&l
( I%$ 3i&) )# id; 1# B04H& tÜWKt tai* *N*#0&WKBgW#
a&ülftM* to t&wk idWPt #w* (K%9B%wp*d i#it&k t&w» %8%aam%>o& aPorirad
ifib*%%tl(%&#
]8#*w&# t&w& «gwpliawâ f%M*gwa8&#y *kt %%M&oiww&8* iK&Il
be Bldk^itlar IcwM*# l&wa# IBao %%at%wMkI d%M»q%ww&oy <>f t&w» i%H»$
m%%aa&H»a TdW%r*ddW%B agfatamk»
jlIt&M5ua)& t&M» daegplayg bw&* *K%aa s&fÊüw&t <*& t&w» $HWpf%m39à*B*a
4)f lBbo lacKb&I agFeiMM#*
la» %&> o<%38l(&&r%d*lo i&r%%%r 3ba twde*
i*y& t&w& agypllak# iüreg%w%nagr to
t&se xw&tgom&l jRpoqpw&Bdgr
o f iBbo zaodaül agnGt#@& Wbwan ta%# {&B9pdba& jka twüllaMnea l&o t%* vsnry
m aall*
ïBbo dam%pl%y& iai twMBb tOie la&dCIl agn&t%H& *o&& lib * %%&&$%&»%%%%»
1^3
OO
OsZ
o .ll
0 ,6
0 .Ô
o)
=
h o
/.2
hU
F r < z c j^ U (2 n c j
I G
/8
R o i i o
h-3 • Resonance D iagram o f
F o rc e d V i b r a t i o n w i t l i V is c o u s Damping » Showing The
iï,f f e c t o f Damping on F re q u e n c y R a tio a t R esonance,
-2.0
jUf aagr#
iBbawi auwsBBWül 4w>
p*%%po3r&loa&#l*
]Ct #a%o%jU& %w*
Beta# th a t p##&iotia& fo r #b# behavior o f tb * proto»typ*
fro # tb# p«rfor#*B@* o f tb * BB&*I »yotm& a#n iab%ylx*aww&*
QBdor tb l# çoBâltloB#
A ll th&#« feotorm j%#% ao&t&omod «blob & ff#ot tb * per#
formanoe o f th6 modal ayetem may bo p a rtia lly or fa ily
:a3&dlBKlj»@kâ 6dl*89wB%* tpgr iabw>ggp#*t%i<>#Cl (N)ii@üldleü*aLtjLo*% os* Ibgr ]***&:&%%&
jK*qBMKM3iP#*gM8K%l%8 31%
% b3%@ cwaciBrLüPuicrbjLf):! (>jT tJi* lakatlal agsrartwiBt f%K#»
j&BOpiÜ&wawp taaad&ljGf; Bmaiplc#
?#»2! ikgnPOPcypGPdLedb**
IBB;** S%k>dbB3L i8grarbOB&, *«"# &jba&*» 1G%w*
dPa&GHgfaaKowogr if*%r4E*k*; iedL#& t8%*& #K%WBaaMt <adf t&%#» jdbuauft: 43jL#a%*1&#r* jtik
%%111 jdtkGHiF #w9q?*%eH)jLaLb1L<» (S&waaaggMk <3üT
3&#8pgf%y%#s9LBw&4t ocP tiaa» %ac*dbB3L
at,f3tM3%& jPoa* *& aijLr&it» ja&waamge* (%f Sasw* aübawlMb djlaB#1ber*
SDOOM»;» iodf gpsibolasaE ikdMOB&dLtdLifljbgr aawadt
JBtmr
i>€oeüRc%e#88ücw8*p <owf i8%(*
3aK>dbB& agr(;1&8*a, jit: la* dksaiiiPtadl t%c> **€)loot% tb l# i#dl3%& jPo:r tdbw)
G@aw*l*t
iB&aat 8%ewà&3l ja3F%rG%*B%*
!%(*%%) f%8üP(Kr#kb:l4> (K):%d&t;loa sasggr dk3u*& Tb<& (OWbtwodlzmk* *%>%* ik&k#*
lacwckal i&#*9r& %%y gtei&i%%jai% %
%
%
> iL%&@a&gkdb&3L a&yaikwBt iKlGki %awtGU*4"lj54*%*kjl<&*
ftBP 4%&>@rt*
aüboü&xl Ibi» luww&dl
jgatt; ]L#Bp%s<* #BWwGdl8y&##* «BawadLl aaauBW&*<la3aMp4bjl@w*
*1 a&a&BkdbMP 2%K>db&l
][t jla %%#HOk&*%sH*apgr jl%%
tao»
41 (BGHawl ]pqp<y%%3G?t%l<%%i iOGwl
ei
jLxi
ITiu) 2%P()&W)8€M& 2»3j;*& 4&af IPomgti* <%cK0d%i'O&
JMk&dk*! i98r#ibM#B&#4*"""
3L& *& i%>%3rjLi%3 tdbM* torqp**» Into tab*» ]%K)dbB& ocP ai adbw&j*# gqsnadMWOkt
jLt iLe 3*0Hgti*jp<»dl l&o» zagdkB» ljadl#apdLdb**k3L
f%*%* ip&%<legw* $%]#%#%**#*
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& og?:33jF tab*» c*>a***»«qpM@%w3Wl*%g laogpqpoK* t%> ây&cai aaaw»#;
jia t&se
<%** 4&
]P4Hp]p8i9(Mnd:iJcy5
aKpgr#üDy»8%a%%Bdb*
Bk&a»jLrw;aftjl& (wowl %&*** ag*w& tx>*qp%#w* oof 4*%%cyln*
<%yCULcw&e%' a%üw#t 1b<» xasid#iNdltab #i ikeqpâkSNad&e» <%SB& ftnr *&awB&& agrlia"»
j&asp*
Ï15%*ü*<» iBWKBà* 3%8%3r i%#k BioMatM&di *9%k *k ladkcysl# dbpdltMext la&uBJpl;
abb %%r<%gHa** ip&WBw*** %%)]L*jbloa t&o awaudbi *»#%*%%*
rtuuBt; Is*»
tw&ioGws jlii isetl&ijQa; tag* iWbw» <B*a&at aw* laba&t 18%* 0&&eüp*&gM&e%ÿdL#ibjL<H# (OdP
taba*
awB&jLcM* aaeKgrTb*» 3*<*tw*jba*»d «&# IGo labw* jC^Li'lng; <)#&#»**
$HB& tdbe* ]p*s*4&aLa%i3b&3P i&3*%q%ii@p*B%e334* <%f 1Kbu&4; <%EygjLcw»*
Sg&w& awBB* la&iawgl; lowKzipgrijQi; iPLll iakw» 1%09&qpwaf*gpopcN3b&ekl%%gE <s*Baw#
ij* 48apdùoM&&Tbgr 8%%*» %aot*>%*-<33*lif4&a*3rart@Bi*
2&**l3ig; :fo3J&epRR%3P# i#3ÜLl
Tbo TWj*€Ha 3Ü& idbu&a* lawtcdb&a&aBi Ibo1s%*@aiaRtlttibkia» asDtdLcMa (%f tdbx» eg***
teo tabd* eaoasljQ*» i8gr3L&%3dW@3&]8Bw;@HN* ja*#py&]p#Kt*»3;y#
tw) TuusGd aw# #L jpdLvoti jpoarb oüT tabeaw*
3P#Ke*%3Llj&3L TsdLtBi tab** a*%BkadkiadM;*
]L(XE%s %%)& iNdLIl
isa&dl %acM8i;tw»(K :&%)
3?1L*BKjlthI**
tab** :fo]Llo%f#p8 (wcwi tObo laasgrlas** (sgKljli&db&x* aaai******
ipSPorvildkBKi#
!%%&*; ILaaog; ILjlggbls *#%xe3Liyg** aàp*k
Ibe
lb**
indH**
ipjLdbaailJXar b&%** jflUeacjlblL** <&<>%Da**<&tiL<%EW» 1b4*t9*N**M& t%ba 3%@:l3cw(KW* aaadl
tbw* 4%33vyN&*g;Ma%wajLEy& anasija** cgrljlztdbBa* laa&aw;**# dka tab** %9E>t&e3L
3B& zswagr %%$
tabw*
(OKkXBaakcdkjlcwaai leawak» *adF
3109812 iLjlght; iggMPdkoy;*; i*3J&3L 1b4k (d%ül4& 1&%
> #&%p3Ly t%o laba* %ag>db*I 1*91*#
tmmtha drivlag tarqp* elollar to the Imput obtained fraa
the
m e # a n lm *
%b* #*me and tb#&# folio#**#
ah#u&a be adjuetable to handi# varlou# aprangemoBt ef the
#&&*& ay&te#*
& eketeh *hê%ln& the Id#* of tbl# erB&Rge#
amB&l# provided &&$%$* kk ( P* 34? *&& IbS )*
BOt# to F ij,
iaamde o f at##l rod la reaaoaebi# *1%#
o f appro&lm&t# leagth egeel to the lbe&ght o f the etand*
2b# #*1& b e a rln j* fo r th la ehaft a*y be eeoured on top
#Bd bottom frame# o f the «tend#
Interm ediate ibeae&n* ##*
ppo&t# a r* **qpir#& fo r e tlffn eea and adjustment*
2be pivo t poet 1# mounted In a lin e w ith the model
aymtem*
Follower# mn#t b* lin ed up along the ;plvot ]po#t
and In p a ra lle l w ith the m a*8»lB #rtl* ObannelmarB# of the
model eyetem before engaging the cam#*
2h&# lanm&re# the
proper pha#e re la tio n met up la 3he earn# on the cam dbaft*
(3)
Figure#
a* b, c dbo# the aaeeWbly o f the cam shaft
and the p ivo t poet o f the emlng follow ere*
Flgwr* d the*#
the fle x ib le connection between #&* fciio w er and the &&##*
In e rtia channel-arm o f the model ayatem#
Oi)
2%B»i%B3%w#cf b#l#B#la& the model When the eammdrlv*
1 kl
d r iv i n g
s h a ft
follower
pivot post
a
. s h a ft /
bearing
(b )
model
system
/Stand
i’ ig * i|l|, - Scheme o f Cam—S h a f t A rran gem ent*
3J4S
follow er
sw ing f o l l o w e r
m a s s - in e r t ia c h a n n e l
arm o f m odel system
s h a f t o f th e
m odel system
F ig * [li!. -
d
-
Scheme o f The F l e x i b l e
C o n n e c tio n b etw een The C a m -F o llo w e r and The M a s i n e r t i a
C h a n n e l-a rm o f Ih e M odel S ystem .
iW
(jg IbwadLBys
lyjldkBd <%ki iBkw$
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atiaS** iOdP t&ie BGCNga»! **3rat#Ba#
4» ibdb#*"
ipod Bgggr Tbt* TaaKkd 1%) <%;%%%%*<*%staws&i jpailar ,83* ;ft>]LIo*p*3p* 1*0 iBbaadb
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a ada&sli* aw #
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Sooom eaittem , 2St|^.
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te W o a itlw , Wk%
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teWmW. C tatestitm tegtm a " ,
M te m Piibltehts^ Co*s»„ v m %«%,.
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