hydrostaticsfluid prac report
TRANSCRIPT
8/20/2019 HydrostaticsFluid Prac Report
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Student Name Student Number C.Munsamy 21416311R.Naidoo 21410445S.Lutchmiah 21350006P.Mthembu 21512087.Moyana 21517171C.M.Mto!o 21520141
"nt#oduction
Hydrostatic pressure is, the pressure exerted by a fuid at
equilibrium due to the orce o gravity. A fuid in this condition is
known as a hydrostatic fuid. So our Hydrostatic pressure lab was
to determine the hydrostatic pressure o water on a fat surace.
Adding weight and then lling the tank with water to the point
where the apparatus was in equilibrium. So we can calculate theorce on the fat surace using the given equations.
Abstract
$he e&'e#iment sho(s the hyd#ostatic th#ust actin) on an ob*ect in a +uid
,(ate#-. ie#ent de'ths (e#e #eco#ded as the (ei)hts (e#e measu#ed.
$he system sta#ted at e/ui!ib#ium o# each indiidua! #eco#ded (ei)ht.
Aim
!uid
Mechanics ""
yd#ostatics
#at Co'y
#ou' 8 Monday
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• $o dete#mine hyd#ostatic th#ust actin) on a '!ane su#ace (hen the
su#ace is 'a#tia!!y subme#)ed and u!!y subme#)ed in (ate#
• ete#mine the 'osition o !ine o action
Apparatus
• $he 112 yd#ostatic P#essu#e ''a#atus
• ate# 9u)
• Measu#in) bea:e#
• Measu#in) system
• ate#
• Set o masses
• Len)th o sma!! bo#e tubin)
Procedure1. dd "nitia! masses and add (ate# to the system. ;/ui!ib#ium must be
#eached.2. $a:e #eadin)s o tube and mass3. Re'eat the '#ocess by addin) die#ent masses to the han)e#.
;/ui!ib#ium must be #eached beo#e #eco#din) mass and de'th4. ate# shou!d be added #om time to time to :ee' system in
e/ui!ib#ium
Results
Readings
Readin) e'th ,mm- Mass ,)-1 <8.5 2002 105.5 230
3 117.5 2804 122.5 3005 12< 3306 141 3807 146.5 4008 154 430< 167.5 480
Calculations
!ormulae or" #using an example o $%%g or each&
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Hydrostatic Thrust
F = ρg bd
3
2
F =1000∗9. 81∗0 .075∗0 .0985
3
2
F = 3.!"
#$perimental Centre o% Pressure
h' ' =
mgL
F
h' ' =0 .2∗9 .81∗0 .275
3 .569
h&= '.(() m
*easured Turning *oment
' ( h) * !
' ( %.++$ * -./
' ( %.-/ 0m
Theoretical Centre o% Pressure
h' ' = H −
d
3
h' ' =0.2−
0.0985
3
H11( %.+2$ m
Turning *oment
' ( h)* !
' ( %.+2$ *-./
' ( %./2 0m
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+iscussion $he o#ce a''!ied in the system e#tica! ace o buoyant mate#ia! counte# acts
the mass added to the han)in) a#m. So (e :no( that i (e moe a(ay #om the
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sea !ee! the '#essu#e (i!! chan)e eithe# (ith ai# o# (ate#. So in ou# e&'e#iment
a!so chan)e in '#essu#e because o the (ei)ht o the (ate# aboe and buoyant
o#ces c!ea#!y sho( the '#o'e#ties o (ate#. $he (ate# '#essu#e (as so hi)h that
(e add the mass 50 ) to 430) een sti!! /uad#ant (as ab!e to su''o#t it in static
e/ui!ib#ium. So the idea !et us to be!iee that the cu#ed a#ea a!!o(s o# a !a#)e#
su#ace (ith (hich the (ate# can act u'on o# !ess chan)e in de'th.
Recommendationsensity (as ta:en as 1000 :).m3 ho(ee# this density on!y a''!ies to 4
e)#ees Ce!sius Readin)s (e#e ta:en on a day (ith much hi)he# tem'e#atu#e
and density (ou!d hae been die#ent (hich (ou!d aect the ca!cu!ations.
Re%erences1. #m=e!d Limited 2002 "nst#uction Manua! 116> Rin)(ood am'shi#e.
?24 1@ ;n)!and
2. 9ohn C!ayden Centre Of Pressure htt'ABB(((.*ccii!en)inee#.comBcent#eo'#essu#e.htm