17
Exam 3 Results ! #! $! %! &! '!! '#! '$! !() )('! '!(') ')(#! #!(#) #)(*! *!(*) *)($! $!($) $)()! )!()) ))(%! %!(%) %)(+! +!(+) +)(&! &!(&) &)(,! ,!(,) ,)('!! !"#$ & '()*+(,-./0 123+#435 6789: Approximate Grade Cutoffs 75 100 A 55 – 74 B 35 – 54 C 25 – 34 D 0 – 24 F You can pick them up a/er class today or Wednesday T. S%egler 12/1/2014 Texas A&M University

Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

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Page 1: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Exam  3  Results  

!"

#!"

$!"

%!"

&!"

'!!"

'#!"

'$!"

!()"

)('!"

'!(')"

')(#!"

#!(#)"

#)(*!"

*!(*)"

*)($!"

$!($)"

$)()!"

)!())"

))(%!"

%!(%)"

%)(+!"

+!(+)"

+)(&!"

&!(&)"

&)(,!"

,!(,)"

,)('!!"

!"#$%&%'()*+(,-./0%123+#435%%6789:%

Approximate  Grade  Cutoffs  Ø  75  -­‐  100  A  Ø  55  –  74  B  Ø  35  –  54    C  Ø  25  –  34  D  Ø  0  –  24  F      

You  can  pick  them  up  a/er  class  today  or  Wednesday  T.  S%egler                12/1/2014            Texas  A&M  University  

Page 2: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Chapter  14  

T.  S%egler                12/1/2014            Texas  A&M  University  

Today    •  Simple  pendulums    •  Physical  pendulums    •  Ch  14  Examples  

Start  Ch  15  (if  we  get  to  it)  

Last  Time  

•  Simple  harmonic  mo%on  of  a  mass-­‐spring  system  

•  Differen%al  equa%ons  and  SHM  

•  Oscilla%ons  in  terms  of  amplitude,  period,  frequency  and  angular  frequency  

•  Simple  harmonic  mo%on  using  energy  

Page 3: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

To  double  the  total  energy  of  a  mass-­‐spring  system  oscilla%ng  in  simple  harmonic  mo%on,  the  amplitude  must  increase  by  a  factor  of  

A. 4.

B.

C. 2.

D.

E.

=2 1.414.

=4 2 1.189.

=2 2 2.828.

0

02

0

( ) cos( )( ) sin( )

( ) cos( )

x t A tv t A ta t A t

ω φ

ω ω φ

ω ω φ

= +

= − +

= − +

21

pend

ff T

mgd gI L

ω π

ω

=

=

= =

12kA2 = 1

2mv2 + 1

2kx2 = const.

Clicker  QuesEon  Review  from  last  Monday    

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 4: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

SHM  and  Pendulums  

•  For  the  physical  pendulum  the  CoM  is  a  distance  d  from  the  pivot,  then  the  torque  at  an  angle  θ  is:    

! = !d(mgsin" )

•  Using  the  small  angle  approxima%on  we  obtain:  

! = !dmg" so   I! ! "dmg"

•  Comparing  to  the  SHM  equa%on  again  gives:  

2

2

1 22

d mgddt I

mgd mgd If TI I mgd

θα θ

ω ππ

⎛ ⎞= = −⎜ ⎟⎝ ⎠

⇒ = ⇔ = ⇔ =

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 5: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

SHM  and  Pendulums  

•  The  simple  pendulum  is  a  special  case  of  the  physical  pendulum.    •  All  the  mass  is  located  at  a  point  aTached  to  the  end  of  string  of  length  L.      

Using  this  d  =  L  and  I  =  mL2        

2

mgd mgL gI mL L

ω = = =

! =gL! f = 1

2"gL!T = 2" L

g

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 6: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Wri%ng  down  Newton's  Second  Law  in  the  x  direc%on  for  some  system  results  in  the  equa%on  on  the  right.  What  is  the  oscilla%on  frequency  of  this  system?    

a2 d2xdt2

= !b2xa)  a/b  b)  a*b  c)  b/a    

Prelecture:  Physical  Pendula  Problem  1    

T.  S%egler                12/1/2014            Texas  A&M  University  

Fx =max

Fx =md 2xdt2

d 2xdt2

+! 2x = 0

Page 7: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Prelecture:  Physical  Pendula  Problem  2  

A  uniform  s%ck  and  a  mass  on  a  string  are  used  to  make  two  pendula  that  have  the  same  length.    Which  one  swings  with  the  longer  period?  

a)  the  mass  on  the  string  b)  the  s%ck  c)  can't  tell  without  knowing  how  the  masses  compare    

T.  S%egler                12/1/2014            Texas  A&M  University  

! =mgdI

=mgLmL2

=gL

T = 2!"

=4! 2Lg

! =mgdI

=mgL13mL2

=3gL

T = 2!"

=4! 2L3g

(a)  

(b)  

Page 8: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Checkpoint:  Physical  Pendula  Problem  1  

A  simple  pendulum  is  used  as  the  %ming  element  in  a  clock  as  shown.  An  adjustment  screw  is  used  to  make  the  pendulum  shorter  (longer)  by  moving  the  weight  up  (down)  along  the  sha_  that  connects  it  to  the  pivot.    If  the  clock  is  running  too  fast,  the  weight  needs  to  be  moved  a)Up  b)Down    

T.  S%egler                12/1/2014            Texas  A&M  University  

T = 2! Lg

Page 9: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Checkpoint:  Physical  Pendula  Problem  2  

A  torsion  pendulum  is  used  as  the  %ming  element  in  a  clock  as  shown.  The  speed  of  the  clock  is  adjusted  by  changing  the  distance  of  two  small  disks  from  the  rota%on  axis  of  the  pendulum.    If  we  adjust  the  disks  so  that  they  are  closer  to  the  rota%on  axis,  the  clock  runs  a)  faster  b)  slower    

! ="I

f = 12#

"I

T = 2# I"

Angular  SHM:   κ  =  torsion  constant  

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 10: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Checkpoint:  Physical  Pendula  Problem  3  Consider  the  two  pendula  shown  above.  In  Case  1  a  s%ck  of  mass  M  is  pivoted  at  one  end  and  used  as  a  pendulum.  In  Case  2  a  point  par%cle  of  mass  M  is  aTached  to  the  center  of  the  same  s%ck.    In  which  case  is  the  period  of  the  pendulum  the  longest?  a)  Case  1  b)  Case  2  c)  Same    

T.  S%egler                12/1/2014            Texas  A&M  University  

! =mgdI

T = 2!"

= 2! Imgd

T1 = 2!

13mL2

mg L2

= 2! 2L3g

T2 = 2!

13mL2 +m L

2!

"#

$

%&

2!

"

##

$

%

&&

2mg L2

= 2! 7L12g

Page 11: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Damped  OscillaEons  

•  Real-world systems have some dissipative forces that decrease the amplitude.

•  The decrease in amplitude is called damping and the motion is called damped oscillation.

•  The figure at the right illustrates an oscillator with a small amount of damping.

•  The mechanical energy of a damped oscillator decreases continuously.

•  When , the system is critically damped and if b is larger than this it is overdamped

•  A critically or overdamped oscillator returns to equilibrium without oscillating.

b = 2 km

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 12: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Example  Pendulum  on  Mars  (14.48)    

A  certain  simple  pendulum  has  a  period  on  the  earth  of  1.60  s.  What  is  its  period  on  the  surface  of  Mars  where  gravity  is  gmars  =  3.71  m/s2?    

0

02

0

( ) cos( )( ) sin( )

( ) cos( )

x t A tv t A ta t A t

ω φ

ω ω φ

ω ω φ

= +

= − +

= − +

21

pend

ff T

mgd gI L

ω π

ω

=

=

= =

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 13: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

A  simple  pendulum  consists  of  a  point  mass  suspended  by  a  massless,  unstretchable  string.  

If  the  mass  is  doubled  while  the  length  of  the  string  remains  the  same,  the  period  of  the  pendulum  

A.  becomes  4  %mes  greater.  

B.  becomes  twice  as  great.    

C.  becomes  greater  by  a  factor  of              .    

D.  remains  unchanged.  

E.  decreases.  

2

Clicker  QuesEon  

0

02

0

( ) cos( )( ) sin( )

( ) cos( )

x t A tv t A ta t A t

ω φ

ω ω φ

ω ω φ

= +

= − +

= − +

21

pend

ff T

mgd gI L

ω π

ω

=

=

= =

12kA2 = 1

2mv2 + 1

2kx2 = const.

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 14: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Example  Physical  pendulum  (small  angle  approxima%on)(14.54)    

A  1.80  kg  monkey  wrench  is  pivoted  0.250  m  from  its  center  of  mass  and  allowed  to  swing  as  a  physical  pendulum.  The  period  for  small  angle  oscilla%ons  is  0.940  s.      a)  What  is  the  moment  of  iner%a  of  the  wrench  about  an  axis  through  the  pivot?  

b)  If  the  wrench  is  ini%ally  displaced  0.400  rad  from  its  equilibrium  posi%on,  what  is  the  angular  speed  of  the  wrench  as  it  passes  through  the  equilibrium  posi%on?  

0

02

0

( ) cos( )( ) sin( )

( ) cos( )

x t A tv t A ta t A t

ω φ

ω ω φ

ω ω φ

= +

= − +

= − +

21

pend

ff T

mgd gI L

ω π

ω

=

=

= =

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 15: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Example  Physical  pendulum  (14.57)    

The  two  pendulums  shown  each  consist  of  a  uniform  solid  ball  of  mass  M  supported  by  a  rigid  massless  rod,  but  the  ball  for  pendulum  A  is  very  small  compared  to  that  of  pendulum  B.  Find  the  period  of  each  pendulum  for  small  displacements.  Which  ball  takes  longer  to  complete  a  swing?  

0

02

0

( ) cos( )( ) sin( )

( ) cos( )

x t A tv t A ta t A t

ω φ

ω ω φ

ω ω φ

= +

= − +

= − +

21

pend

ff T

mgd gI L

ω π

ω

=

=

= =

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 16: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Example  Pendulums  and  collisions(14.95)    In  the  figure  the  upper  ball  is  released  from  rest,  collides  with  the  sta%onary  lower  ball,  and  s%cks  to  it.  The  strings  are  both  50.0  cm  long.  The  upper  ball  has  mass  2.00  kg,  and  ini%ally  10  cm  higher  than  the  lower  ball  (mass  3.00  kg).  Find  the  frequency  and  maximum  angular  displacement  of  the  mo%on  a_er  the  collision.    

0

02

0

( ) cos( )( ) sin( )

( ) cos( )

x t A tv t A ta t A t

ω φ

ω ω φ

ω ω φ

= +

= − +

= − +

21

pend

ff T

mgd gI L

ω π

ω

=

=

= =

T.  S%egler                12/1/2014            Texas  A&M  University  

Page 17: Exam3Results - Physics and Astronomy at TAMUpeople.physics.tamu.edu/tyana/PHYS218/files/Lect_26_12-1-14_post.pdf · DampedOscillaons+ • Real-world systems have some dissipative

Example  Energy  and  momentum  in  SHM  

A  block  of  mass  M  is  aTached  to  a  horizontal  spring  with  spring  constant  k  and  is  moving  in  SHM.  As  it  passes  through  its  equilibrium  point  a  lump  of  puTy  of  mass  m  is  dropped  from  a  small  height  and  s%ck  to  it.    Find  the  new  amplitude  and  period.  

T.  S%egler                12/1/2014            Texas  A&M  University  

21

pend

ff T

mgd gI L

ω π

ω

=

=

= =

12kA2 = 1

2mv2 + 1

2kx2 = const.