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8/18/2019 05. Physics B 2009 Free Response (1)
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8/18/2019 05. Physics B 2009 Free Response (1)
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Problem B-1
Problem B-2
Problem B-3
Problem B-4
Problem B-5Problem B-6
2009 AP Physics B
END
Problem B-7
Grade Distributions
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2009 Grade Distributions
14.9
5
18.6
4
27.2
3
18.3
2
20.9
1
62,702 Eams
!ean Grade " 2#$6
2009 AP Physics B
!enu
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%n an e&eriment, students are to 'al'ulate t(e s&rin) 'onstant k o* a
+erti'al s&rin) in a small um&in) to t(at initiall rests on a table# .(en
t(e s&rin) in t(e to is 'om&ressed a distan'e x *rom its un'om&ressed
len)t( L0 and t(e to is released, t(e to& o* t(e to rises to a maimum
(ei)(t h abo+e t(e &oint o* maimum 'om&ression# /(e students re&eatt(e e&eriment se+eral times, measurin) h it( obe'ts o* +arious masses
ta&ed to t(e to& o* t(e to so t(at t(e 'ombined mass o* t(e to and added
obe'ts is m . /(e bottom o* t(e to and t(e s&rin) ea'( (a+e ne)li)ible
mass 'om&ared to t(e to& o* t(e to and t(e obe'ts ta&ed to it#
P(si's B-1 15 &oints
2009 P-B Eam
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a 3 &oints
Deri+e an e&ression *or t(e (ei)(t h in
terms o* m, x , k , and *undamental
'onstants#
221m)(Ener)-#ons
m)2
(
2
=
P(si's B-1 15 &oints
1 &t# onser+ation o* Ener)
1 &t# orre't Ener) E&ression
1 &t# ol+in) *or (
2009 P-B Eam
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.it( t(e s&rin) 'om&ressed a distan'e x " 0#020 m in ea'( trial, t(e
students obtained t(e *olloin) data *or di**erent +alues o* m#
b i# 2 &oints
.(at uantities s(ould be )ra&(ed so t(at t(e slo&e o* a best-*it strai)(t
line t(rou)( t(e data &oints 'an be used to 'al'ulate t(e s&rin) 'onstant k 8
P(si's B-1 15 &oints
(
1 +s#mor
m
1 +s#(Plot
2 &t# E&ression
(
1+s#m
m
1+s#( ⇔
2009 P-B Eam
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.it( t(e s&rin) 'om&ressed a distan'e x " 0#020 m in ea'( trial, t(e
students obtained t(e *olloin) data *or di**erent +alues o* m#
b ii# 2 &oints
ill in one or bot( o* t(e blan 'olumns in t(e table it( 'al'ulated +alues
o* our uantities, in'ludin) units#
1:m )-1
50
33
25
20
17
1:( m-1
2#0
2#9
3#6
5#3
5#6
P(si's B-1 15 &oints
1 &t# illin) table it( 'orre't +alues#
1 &t# orre't ;nits#
2009 P-B Eam
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' 4 &oints
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d 2 &oints
;sin) our best-*it line,
'al'ulate t(e numeri'al +alueo* t(e s&rin) 'onstant#
0#5
0#4
0#3
0#2
0#1
0 10 20 30 40 50 60
(
1:m
(
∆
1 m
m
1
(lo&es
∆
∆
=
2
2
m020#0
m:s$#9)m0107#02 ⋅=
N:m524 =
P(si's B-1 15 &oints
1040
10#042#0
=
)m0107#030
32#0⋅
m)2
(
2
=
2
)(m2 =
2
)slo&e2 =
1 &t# al'ulatin) t(e lo&e
1 &t# orre't >alue *or &rin) onstant
2009 P-B Eam
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e 2 &oints
Des'ribe a &ro'edure *or measurin) t(e (ei)(t h in t(ee&eriment, )i+en t(at t(e to is onl momentaril at t(at
maimum (ei)(t
;se a timer to measure t(e time t(e to is in t(e air#al'ulate t(e maimum (ei)(t rea'(ed usin) t(is time#
P(si's B-1 15 &oints
2 &t# orre't, om&lete Pro'edure
2009 P-B Eam
!enu
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/o small obe'ts, labeled 1 and 2 in t(e dia)ram abo+e, are sus&ended
in euilibrium *rom strin)s o* len)t( L# Ea'( obe't (as mass m and
'(ar)e ?Q . ssume t(at t(e strin)s (a+e ne)li)ible mass and are
insulatin) and ele'tri'all neutral# E&ress all al)ebrai' ansers interms o* m, L, Q, , and *undamental 'onstants#
P(si's B-2 10 &oints
2009 P-B Eam
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a 3 &oints
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b 2 &oints
Deri+e an e&ression *or t(e ele'tri' &otential at&oint , s(on in t(e dia)ram at t(e to& o* t(e
&a)e, (i'( is mida beteen t(e '(ar)ed
obe'ts#
P(si's B-2 10 &oints
22
11
r
r
>
r
A2> =
θ
sin=
A2
1 &t# (oin) ield ontributions#
1 &t# orre't E&ression
;sin) Gi+en Auantities
2009 P-B Eam
r
θsin=r
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' 2 &oints
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d 3 &oints
;sin) t(e 'onditions o* euilibrium, ritebut do not
sol+eto euations t(at 'ould, to)et(er, be sol+ed*or and t(e tension T in t(e le*t-(and strin)#
/
m)
E
θ
Esin/
m)'os/
2
2
r
A
2
2
sin=2
A
θ
=
P(si's B-2 10 &oints
1 &t# /C " E#
1 &t# / " m)#
1 &t# tatin) t(e /o Euations
;sin) Gi+en Auantities
m)'os/ =
2
2
sin=2
Asin/
θ
==
2009 P-B Eam
θsin=2r
r
!enu
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metal rod o* mass 0#22 ) lies a'ross to &arallel 'ondu'tin)
rails t(at are a distan'e o* 0#52 m a&art on a tableto&, as s(on in
t(e to& +ie abo+e# 3#0Ω
resistor is 'onne'ted a'ross t(e le*tends o* t(e rails# /(e rod and rails (a+e ne)li)ible resistan'e but
si)ni*i'ant *ri'tion it( a 'oe**i'ient o* ineti' *ri'tion o* 0#20#
/(ere is a ma)neti' *ield o* 0#$0 / &er&endi'ular to t(e &lane o*
t(e tableto strin) &ulls t(e metal rod to t(e ri)(t it( a
'onstant s&eed o* 1#$ m:s#
P(si's B-3 15 &oints
2009 P-B Eam
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a 3 &oints
al'ulate t(e ma)nitude o* t(e'urrent indu'ed in t(e loo& *ormed
b t(e rod, t(e rails, and t(e resistor#
% ε
=
Ω 0#3
m:s1#$m0#52/$0#0 25#0
P(si's B-3 15 &oints
B=+=
1 &t#
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b 4 &oints
al'ulate t(e ma)nitude o* t(e
*or'e reuired to &ull t(e rod to t(eri)(t it( 'onstant s&eed#
m) * µ 2m:s9#$)0#2220#0 N0#43
B%=B = m0#520#25/$0#0 N0#10
B* N0#10N0#43 N0#53
P(si's B-3 15 &oints
1 &t# or'e o* ri'tion
1 &t# orre't !a)neti' or'e
1 &t# ddin) t(e /o or'es
1 &t# orre't anser
2009 P-B Eam
P( i B 3 15 i
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' 3 &oints
al'ulate t(e ener) dissi&ated in
t(e resistor in 2#0 s#
PtE =
t %E2
s#023#00#25 2 Ω 0#3$
P(si's B-3 15 &oints
1 &t# Poer-Ener) elations(i&
1 &t# Ele'tri' Poer %2
1 &t# orre't ubstitution
2009 P-B Eam
P( i B 3 15 i t
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d 2 &oints
al'ulate t(e or done b t(e
strin) &ullin) t(e rod in 2#0 s#
+td =
s2#0m:s$#1d =
m6#3d
d. =
m3#6N#540.
9#1. =
P(si's B-3 15 &oints
1 &t# orre't E&ression *or Distan'e
1 &t# orre't ubstitution *or or'e
2009 P-B Eam
P( i B 3 15 i t
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e 2 &oints
om&are our ansers to &arts
' and d# Pro+ide a &(si'ale&lanation *or ( t(e are
eual or uneual#
nser ' does not in'lude or done b *ri'tion#
.or done b *ri'tion dissi&ates ener)#
P(si's B-3 15 &oints
1 &t# .or Done b ri'tion not %n'luded
1 &t# ri'tion Dissi&ates Ener)
2009 P-B Eam
9#1. d
0#3$E '
=
=
!enu
P( i B 4 10 i t
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/(e 'linder 'ontains 2#2 ) o* ater +a&or initiall at a
+olume o* 2#0 m3 and an absolute &ressure o* 3#0 105 Pa#
/(is state is re&resented b &oint A in t(e P> dia)ram
belo# /(e molar mass o* ater is 1$ ), and t(e ater +a&or
'an be treated as an ideal )as#
P(si's B-4 10 &oints
2009 P-B Eam
P( i B 4 10 i t
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a 3 &oints
al'ulate t(e tem&erature o*
t(e ater +a&or at &oint A#
n/P> =
n
P>/ =
H :mol$#31mol122
m#02Pa100#3 33
⋅
H 590
):mol10$1
)2#2n
3mol122
P(si's B-4 10 &oints
1 &t# %deal Gas =a
1 &t# orre't Number o* !oles
1 &t# orre't ubstitution
2009 P-B Eam
):mol10$1!
)2#2m
3.
.
=
=
P( si's B 4 10 &oints
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b 1 &oint
al'ulate t(e tem&erature o* t(e ater +a&or at &oint C #
n P>/
=
H :mol$#31mol122m#52Pa100#4 33⋅
H 9$0
P(si's B-4 10 &oints
1 &t# orre't nser and ;nits
2009 P-B Eam
/(e absolute &ressure o* t(e
ater +a&or is in'reased at
'onstant +olume to 4#0 105 Pa
at &oint B, and t(en t(e +olume
o* t(e ater +a&or is in'reased
at 'onstant &ressure to 2#5 m3
at &oint C , as s(on in t(e P> dia)ram# mol122n =
P(si's B 4 10 &oints
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' 3 &oints
Does t(e internal ener) o* t(eater +a&or *or t(e &ro'ess
AI BIC in'rease, de'rease, or
remain t(e same8
JJJJ%n'rease JJJJDe'rease JJJJemain t(e same
usti* our anser
%nternal ener) is &ro&ortional to tem&erature#
P(si's B-4 10 &oints
1 &t# ele'tin) %n'rease
2 &t# orre't usti*i'ation
2009 P-B Eam
H 9$0
H 590
P(si's B 4 10 &oints
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d 3 &oints
al'ulate t(e or done on t(e
ater +a&or *or t(e &ro'ess
AI BIC #
/(e area under t(e 'ur+e re&resents t(e or
done on t(e ater#
>P. ∆
35m#500Pa100#4 100#2
5
P(si's B-4 10 &oints
1 &t# .or Euals rea ;nder ur+e
1 &t# orre't Numeri'al nser and ;nits
1 &t# Ne)ati+e i)n on nser
2009 P-B Eam
!enu
P(si's B 5 10 &oints
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/(ree obe'ts o* identi'al mass atta'(ed to strin)s are
sus&ended in a lar)e tan o* liuid, as s(on abo+e#
P(si's B-5 10 &oints
2009 P-B Eam
P(si's B 5 10 &oints
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a 3 &oints
!ust all t(ree strin)s (a+e t(e same tension8 JJJJ es JJJJ No
usti* our anser#
/(e tension in ea'( strin) de&ends on t(e ei)(t
and buoant *or'e on ea'( obe't#
/(e buoant *or'e on a submer)ed obe't de&ends
on t(e obe'tFs +olume#
P(si's B-5 10 &oints
1 &t# ele'tin) No
2 &t# orre't usti*i'ation
2009 P-B Eam
P(si's B 5 10 &oints
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olume
1 &t# orre't nser
2009 P-B Eam
P(si's B-5 10 &oints
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' 2 &oints
al'ulate t(e densit o* t(e liuid#
B =
>)
B
= =
23 m:s$#9m5-100#1
N12#0
=
3):m1200
P(si's B-5 10 &oints
1 &t# orre't ubstitution
1 &t# orre't nser
2009 P-B Eam
B
N12B =
P(si's B-5 10 &oints
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d 2 &oints
ome o* t(e liuid is no drained *rom t(e tan untilonl (al* o* t(e +olume o* obe't is submer)ed#
.ould t(e tension in t(e strin) to (i'( obe't is
atta'(ed in'rease, de'rease, or remain t(e same8
JJJJ %n'rease JJJJ De'rease JJJJ emain t(e same
usti* our anser#
=ess liuid is dis&la'ed t(ere*ore t(e buoant *or'e is less
Bm)/
P(si's B-5 10 &oints
1 &t# ele'tin) %n'rease
1 &t# orre't usti*i'ation
2009 P-B Eam
!enu
P(si's B-6 10 &oints
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%n a 'lassroom demonstration, a beam o* 'o(erent li)(t o*
a+elen)t( 550 nm is in'ident &er&endi'ularl onto a &air o* slits#
Ea'( slit (as a idt( w o* 1#2 10 6 m, and t(e distan'e d beteen
t(e 'enters o* t(e slits is 1#$ 10 6 m# /(e 'lass obser+es li)(t and
dar *rin)es on a s'reen t(at is a distan'e L o* 2#2 m *rom t(e slits#
P(si's B-6 10 &oints
2009 P-B Eam
P(si's B-6 10 &oints
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a 2 &oints
al'ulate t(e*reuen' o* t(e li)(t#
λ
* '
λ
'*
m10550
m:s103#0
9
$
KL105#514
=
P(si's B 6 10 &oints
1 &t# &eed-reuen'-.a+elen)t(
1 &t# orre't anser
2009 P-B Eam
m:s100#3'
m105509
9
P(si's B-6 10 &oints
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b 3 &onts
al'ulate t(e distan'e beteen
to ada'ent dar *rin)es ont(e s'reen#
d=m
λ
1m
d
=
λ
=
m10#$1
m10505m#22
5
9
=
m067#0
P(si's B 6 10 &oints
1 &t# %nter*eren'e &osition
1 &t# %nter*eren'e e&aration
1 &t# orre't ubstitution
2009 P-B Eam
λ
" 550 nm L " 2#2 m
d " 1#$ 10 6 m
P(si's B-6 10 &oints
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/(e entire a&&aratus is no immersed in a trans&arent *luid(a+in) inde o* re*ra'tion 1#4#
' 2 &oints
.(at is t(e *reuen' o* t(e li)(t in t(e trans&arent *luid8
KL105#5* 14=
P(si's B 6 10 &oints
2 &t# reuen' Does Not (an)e
2009 P-B Eam
P(si's B-6 10 &oints
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d 3 &oints
Does t(e distan'e beteen t(e dar *rin)es in'rease, de'rease, or
remain t(e same8
JJJJJ %n'rease JJJJJ De'rease JJJJJ emain t(e same
E&lain our reasonin)#
d
=
λ
=
is &ro&ortional to t(e a+elen)t( nad
t(e a+elen)t( de'reases in t(e *luid#
P(si's B 6 10 &oints
1 &t# ele'tin) De'rease
2 &t# orre't easonin)
2009 P-B Eam
!enu
P(si's B-7 10 &oints
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&(oton o* a+elen)t( 250 nm ee'ts an ele'tron *rom a metal#
/(e ee'ted ele'tron (as a de Bro)lie a+elen)t( o* 0#$5 nm#
a 3 &oints
al'ulate t(e ineti' ener) o* t(e ele'tron#
2
m+H
2
=
m+
(=
λ
m
(
+
2
m
(m
2
λ
=
2
2
m2(H λ
2931
234
m10#$50)1011#92
s1063#6
⋅
=
103#3 19=
P(si's B 7 10 &oints
1 &t# orre't ubstitution
o* a+elen)t( *or >elo'it
1 &t# orre't ubstitution o* Plan'Fs onstant
1 &t# orre't ubstitution o* Ele'tron !ass
2009 P-B Eam
P(si's B-7 10 &oints
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b 3 &oints
ssumin) t(at t(e ineti' ener) *ound in a is t(e maimum ineti'
ener) t(at it 'ould (a+e, 'al'ulate t(e or *un'tion o* t(e metal#
&(oton o* a+elen)t( 250 nm ee'ts an ele'tron *rom a metal#
/(e ee'ted ele'tron (as a de Bro)lie a+elen)t( o* 0#$5 nm#
φ
(* H
H (* H ('
λ
103#3m10502
m:s103#0s1063#6 199
$34
=
107#419
=
&
1 &t# P(otoele'tri' E**e't
1 &t# orre't ubstitution o* P(oton .a+elen)t(
1 &t# orre't ubstitution o* ('
1 &t# orre't ;nits in Parts a and b2009 P-B Eam
P(si's B-7 10 &oints
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' 3 &oints
/(e in'ident &(oton as 'reated (en an atom underent an ele'troni'
transition#
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