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    PIONEER JUNIOR COLLEGEPromotional Examination

    PHYSICS 9646/02Hig!r 2

    Paper 2 Structured Questions

    7 October 2009

    2 o"r# $% min"t!#Candidates answer on the Question Paper.No Additional Materials are required.

    RE&' (HESE INS(RUC(IONS )IRS(

    rite !our na"e# class and inde$ nu"ber on all the wor% !ou hand in.rite in dar% blue or blac% pen.&ou "a! use a so't pencil 'or an! dia(ra"s# (raphs or rou(h wor%in(.

    )o not use staples# paper clips# hi(hli(hters# (lue or correction 'luid.

    Answer allquestions.

    At the end o' the e$a"ination# 'asten all !our wor% securel! to(ether.*he nu"ber o' "ar%s is (i+en in brac%ets , - at the end o' each question or part question.

    )or Examin!r*# U#!

    $ 7

    2 /

    + 1

    4 0

    % 0

    6 2

    ,

    - 1

    (otal 90

    *his docu"ent consists o' 22printed pa(es.

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    Nam! Cla## In!x N"m1!r

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    'ata

    speed o' li(ht in 'ree space# /000.3 =c " s4

    per"eabilit! o' 'ree space# 70 01

    = 5 "4

    per"itti+it! o' 'ree space# 20 0/./ = 6 "4

    ( )( ) 903 = 6 "4

    ele"entar! char(e# 900. =e C

    the Planc% constant# 3103. =h 8 s

    uni'ied ato"ic "ass constant# 270. =u %(

    rest "ass o' electron# 30.9 =e

    m %(

    rest "ass o' proton# 2707. =pm %(

    "olar (as constant# 3./=R 8 4 "ol4

    the A+o(adro constant# 23002. =A

    N "ol4

    the :olt;"ann constant# 2303/. =k 8 4

    (ra+itational constant# 07. =G N "2 %(42

    acceleration o' 'ree 'all# /.9=g " s42

    )orm"la!

    2

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    uni'or"l! accelerated "otion# 2

    2

    atuts +=

    asuv 222+=

    wor% done onb! a (as# VpW =

    h!drostatic pressure# ghp =

    (ra+itational potential#r

    Gm=

    displace"ent o' particle in s.h.".# txx sin0=

    +elocit! o' particle in s.h.".# tvv cos0=

    22

    0

    xx =

    resistors in series# ...2 ++= RRR

    resistors in parallel# ... 2 ++= RRR

    electric potential#r

    QV

    01=

    alternatin( current+olta(e# txx sin0=

    trans"ission coe''icient# ( )kdT 2e$p = where( )2

    2/

    h

    EUmk

    =

    radioacti+e deca!#

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    ? ........................................ ,3-

    2 A tile o' "ass 270 (# initiall! at rest# slides down a roo' 'or a distance o' 3./ " be'ore'allin( o'' the roo'. *he tile e$periences a resisti+e 'orce o' 0.10 N while slidin(. *he roo'is inclined at an an(le o' 2 to the hori;ontal# and its ed(e is 2.3 " abo+e the (roundas shown in 6i(. 2..

    %

    2

    tile

    roo'

    (round

    2.3 "

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    )ig 2$

    a3 Calculate the acceleration o' the tile as it slides down the roo'.

    acceleration ? ........................................ " s42 ,2-

    13 )eter"ine the speed o' the tile Bust as it lea+es the roo'.

    speed ? ........................................ " s4 ,2-

    53 )eter"ine the ti"e ta%en 'or the tile to hit the (round a'ter lea+in( the roo'.

    6

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    ti"e ta%en? ........................................ s ,2-

    3 )eter"ine the hori;ontal distance 'ro" the ed(e o' the roo' at which the tile lands.

    hori;ontal distance? ........................................ " ,2-

    + a3 A c!linder with a piston contains 0.00 "oles o' an ideal (as at 000.1 Pa and

    300 . *he (as under(oes 3 processes

    =< e$panded at constant pressure to twice its ori(inal +olu"eD and then=2< co"pressed at constant te"perature to its ori(inal +olu"eD and 'inall!=3< cooled at constant +olu"e to its ori(inal pressure.

    i3 Calculate the ori(inal +olu"e o' ideal (as in the c!linder.

    ,

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    +olu"e ? ........................................ "3 ,2-

    ii3On 6i(. 3.# s%etch the series o' processes =

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    wor% done b! the (as? ........................................ 8 ,2-

    13 i3 )e'ine specific heat capacity.

    ..................................................................................................................................

    ..................................................................................................................................

    ........................................................................................................................... ,2-

    ii3 @n a heatin( e$peri"ent# ener(! is supplied at a constant rate to a liquid in a

    bea%er o' ne(li(ible heat capacit!. *he te"perature o' the liquid rises at 1.0 per"inute Bust be'ore it be(ins to boil. A'ter 10 "inutes all the liquid has boiled awa!.6or this liquid# calculate the ratio o' its speci'ic heat capacit! to its speci'ic latentheat o' +apori;ation.

    ratio ? ........................................ 4 ,3-

    4 a3 6i( 1. shows 'i+e identical car(o bo$es# each o' "ass m# spaced out in a strai(htline on a 'rictionless hori;ontal sur'ace. All 'i+e bo$es are stationar! initiall!.

    )ig 4$

    9

    A : C ) E

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    :o$ A is (i+en a push and it "o+es towards bo$ : at a +elocit! ov . A'ter collidin(

    with bo$ :# bo$ A and : continues to "o+e 'orward until all 'i+e bo$es are touchin(one another and "o+in( at a co""on +elocit!.

    i3 State thepricip!e of coservatio of mometum.

    ..................................................................................................................................

    ..................................................................................................................................

    ........................................................................................................................... ,-

    ii3 E$press the co""on 'inal +elocit! o' the 'i+e bo$es in ter"s o' ov .

    ,2-

    iii3 Calculate the ratio o' the %inetic ener(ies o' the 'i+e bo$es be'ore the collisionto that a'ter the collision.

    ratio ? ........................................ ,-

    13 6i( 1.2 shows the 'i+e bo$es at rest in a strai(ht line on a s"ooth hori;ontal sur'acewith their adBacent 'aces in contact.

    $0

    A : C ) EP

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    ,-

    3 *he car(o bo$es contain brea%able ite"s and are to be brou(ht onto a hori;ontalsur'ace without brea%in( the contents inside. A 'rictionless ra"p F& is added ontora"p PQ with an inclined an(le # where is s"aller than . *his helps to

    reduce the i"pact on the bo$es as the! "o+e 'ro" ra"p PQ to the hori;ontal sur'ace# asshown in 6i(. 1.1.

    )ig 44

    @' the bo$es are released 'ro" the sa"e hei(ht as be'ore# e$plain how the insertiono' ra"p F which has a s"aller (radient# helps to reduce the i"pact on the bo$es.

    .......................................................................................................................................

    .......................................................................................................................................

    .......................................................................................................................................

    ................................................................................................................................. ,2-

    $2

    A:

    C)

    E

    P

    Q

    F

    &

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    % a3 A helicopter tra+ellin( at a hei(ht o' 3000 " abo+e the (round dra(s alon( a 1.0 %("ass A that is suspended 'ro" the helicopter at P with a li(ht ine$tensible cord o'

    len(th 0.0 ". A hori;ontal dra( 'orce "# o' 300 N is e$erted on the "ass as the

    helicopter 'lies at constant speed$*his causes the cord to be inclined at an an(le o' 'ro" the +ertical as shown in 6i(. ..

    )ig %$

    i3 )raw a labelled 'reeGbod! dia(ra" o' all the 'orces actin( on "ass A.

    ,-

    ii3 E$press# in ter"s o' #

    $ the cloc%wise "o"ent due to the wei(ht o' "ass A about point P$

    ,-

    2 the antiGcloc%wise "o"ent due to "# about point P$

    ,-

    $+

    P

    "ass A

    0.0 "

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    iii35ence or otherwise# deter"ine the an(le o' inclination .

    ? ........................................ ,2-

    13 @n the helicopter# a "an detaches the cord at P and allows "ass A to 'all 'reel! awa!

    'ro" the helicopter. At the sa"e ti"e# a si"ilar "ass :# wei(hin( 7.0 %(# waspushed o'' 'ro" the helicopter.

    Mass A attains a +ertical ter"inal +elocit! o' 0/ %" hH soon a'ter lea+in( thehelicopter. Mass : also attains ter"inal +elocit! and continues to 'all +erticall!

    towards "ass A. @t "a! be assu"ed that the +iscous dra( 'orce v# e$perienced b!

    a 'allin( "ass is proportional to 2v # where vis the speed o' the "ass. >pthrust due

    to air "a! be i(nored.

    i3 )eter"ine the ter"inal +elocit! that "ass : would attain assu"in( that itshori;ontal +elocit! is ne(li(ible.

    ter"inal +elocit! ? ........................................ " s4 ,3-

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    ii3 )raw the path ta%en b! "ass A 'ro" the "o"ent it was released till it reaches the(round.

    ,2-

    $%

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    6 A .30 %( bloc% is released 'ro" point A as shown in 6i( .. *he trac% is 'rictionless#e$cept 'or the rou(h sur'ace between : and C# which has a len(th o' .00 ". *he bloc%tra+els down the trac%# hits a sprin( at ) o' 'orce constant k ? 10 N "H# andco"presses the sprin( 0.10 " 'ro" its equilibriu" position be'ore co"in( to rest"o"entaril!.

    )ig 6$

    a3 Calculate the speed o' the bloc% at :.

    speed ? ........................................ " s4 ,2-

    13 Calculate the ener(! stored in the sprin( a'ter the bloc% has co"pressed the sprin('ull!.

    ener(! stored? ........................................ 8 ,2-

    $6

    2.0 "

    A

    :

    )

    C.00 "

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    53 On 6i(. .2# s%etch a labelled (raph to show the +ariation o' the 'orce #e$erted b!the bloc% on the sprin( a(ainst the co"pression o' the sprin(x.

    )ig 62 ,2-

    3 Calculate the ener(! lost due to 'riction# assu"in( all other 'or"s o' ener(! lossesare ne(li(ible.

    ener(! lost? ........................................ 8 ,2-

    !3 5ence# calculate the a+era(e 'rictional 'orce actin( a(ainst the bloc%.

    a+era(e 'rictional 'orce? ........................................ N ,2-

    3 @' the bloc% rebounds and "o+es le'twards past C a'ter the sprin( deco"pressesitsel'# calculate the distance 'ro" C at which the bloc% will 'inall! co"e to rest.

    $,

    x "

    # N

    0

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    distance ? ........................................ " ,2-

    $-

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    , a3 *he (ra+itational 'ield stren(th o' the Earth at its sur'ace is 9./ N %(H.

    Show that

    i3 the acceleration o' 'ree 'all at the sur'ace o' the Earth is 9./ " sH2.

    ,2-

    ii3N %(H

    is equi+alent to " sH2

    in S@ base units.

    ,2-

    13 A satellite o' "ass morbits the Earth o' "ass %and radius Er . *he radius o' the

    orbit is R. *he satellite and the Earth "a! be considered to be point "asses withtheir "asses concentrated at their centres. *he! "a! be assu"ed to be isolated inspace.

    i3 E$plain wh! the satellite does not "o+e in the direction o' the (ra+itational 'orce.

    ..................................................................................................................................

    ..................................................................................................................................

    ........................................................................................................................... ,-

    $9

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    ii3 )eri+e an e$pression# in ter"s o' Er # 'or the radius o' the orbit Rso that the

    an(ular +elocit! o' the satellite is equal to the an(ular +elocit! o' the Earth.E$plain !our wor%in(.

    ,1-

    iii3State two circu"stances under which a satellite at this distance will be a(eostationar! satellite.

    $ ............................................................................................................................

    ..................................................................................................................................

    2 ............................................................................................................................

    .......................................................................................................................... ,2-

    53 As a result o' air resistance# the satellite loses ener(! as it orbits the Earth. E$plainthe e''ect o' this chan(e on

    i3 the radius o' the orbit#

    .......................................................................................................................................

    .......................................................................................................................................

    ................................................................................................................................. ,2-

    ii3 the speed o' the satellite.

    .......................................................................................................................................

    20

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    .......................................................................................................................................

    ................................................................................................................................. ,2-- a3 )e'ine simp!e harmoic motio.

    .......................................................................................................................................

    .......................................................................................................................................

    ................................................................................................................................. ,2-

    13A +ertical sprin( supports a "ass %o' 0./0 %( as shown in 6i(. /.. *he "ass isdisplaced +erticall! upwards b! 2.0 c" and then released. @t reaches the lowestposition in 0.27 s and oscillates in si"ple har"onic "otion.

    )ig -$

    At the point when it is released#

    i3 deter"ine the acceleration o' the "ass %#

    acceleration ? ........................................ " s42 ,3-

    ii3 deter"ine the "a(nitude o' the net 'orce actin( on the "ass# and its direction.

    2$

    %

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    net 'orce? ........................................ N ,-

    direction? ........................................ ,-iii3deduce the tension in the sprin(.

    tension? ........................................ N ,2-

    53 *he sprin( s!ste" in 6i( /. is now connected to a +ariable 'requenc! +ibrator as

    shown in 6i(. /.2.

    )ig -2

    *he +ibrator itsel' has constant a"plitude. As the 'requenc! is +aried# the a"plitudeo' oscillation o' the "ass %(oes throu(h so"e chan(es.

    i3 On 6i(. /.3# s%etch a wellGlabelled (raph to show the +ariation o' a"plitude o'"ass %with the 'requenc! o' the +ibrator.

    22

    %

    Iariable 'requenc! +ibrator

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    )ig -+ ,3-ii3*he pheno"enon which is illustrated in 53can cause considerable en(ineerin(

    proble"s. State one such proble" and su((est a wa! in which it can beo+erco"e.

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    ..................................................................................................................................

    ..................................................................................................................................

    ........................................................................................................................... ,2-

    2+

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