Lecture 2: examples of rigid body kinematics · 2013. 4. 13. · Lecture 2: examples of rigid body...

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Lecture 2: examples of rigid body kinematics forward kinematics problem head impact demo rolling disk intro to project #3 Tuesday, April 9, 13

Transcript of Lecture 2: examples of rigid body kinematics · 2013. 4. 13. · Lecture 2: examples of rigid body...

Page 1: Lecture 2: examples of rigid body kinematics · 2013. 4. 13. · Lecture 2: examples of rigid body kinematics • forward kinematics problem • head impact demo • rolling disk

Lecture 2: examples of rigid body kinematics

• forward kinematics problem• head impact demo• rolling disk• intro to project #3

Tuesday, April 9, 13

Page 2: Lecture 2: examples of rigid body kinematics · 2013. 4. 13. · Lecture 2: examples of rigid body kinematics • forward kinematics problem • head impact demo • rolling disk

robotic arm• Forward Kinematics: prescribe motion of

links AB & BC, calculate motion of C

http://www.nytimes.com/2012/05/26/science/space/space-x-capsule-docks-at-space-station.html?_r=0

j

kiθ1

θ2

Α

B

C

↵AB = ↵BC = Asin(⇡t)rC =vC =

Given:Find:

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robotic arm hw problem

• Inverse Kinematics: given motion of point C, calculate kinematics of links AB & BC

http://www.nytimes.com/2012/05/26/science/space/space-x-capsule-docks-at-space-station.html?_r=0

j

kiθ1

θ2

Α

B

C

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NCAA Football Impacts (Courtesy: Dr. Crisco, Rhode Island Hospital)

Head Impact Telemetry System (HITs)

NIH BRP: Simbex, Brown, Dartmouth,

Virginia Tech

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NCAA Football Impacts (Courtesy: Dr. Crisco, Rhode Island Hospital)

Head Impact Telemetry System (HITs)

NIH BRP: Simbex, Brown, Dartmouth,

Virginia Tech

Tuesday, April 9, 13

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y""

x""

z""

F"

CM"r1""

aCM"

a1"α, ω# single-axis accelerometer

acceleration at CG?

angular acceleration?

Magnitude of Force and Location of Impact?

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• accelerometer measures 1 direction of acceleration only, in direction of orientation!

• how do we obtain accelerations, linear/rotational?

• how do we obtain magnitude and location of impact?

3D kinematics of helmet testing

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Rolling Disk (no slip)

O O’

C

C’θ

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Rolling Disk (no slip)

O O’

C

C’θ

O’C’ θ RcosθRsinθ

Motion of Center (O):s = Rθvo=Rωao=Rα

Motion of Point C:x = s-Rsinθ = R(θ-sinθ)vcx= Rω(1-cosθ)acx=Rα(1-cosθ)+ Rω2(sinθ)

y = R(1-cosθ)vcy= Rω(sinθ)acy=Rα(sinθ)+ Rω2(cosθ)

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Page 10: Lecture 2: examples of rigid body kinematics · 2013. 4. 13. · Lecture 2: examples of rigid body kinematics • forward kinematics problem • head impact demo • rolling disk

Rolling Disk (no slip)

O O’

C

C’θ

rB = rO + rB/O

B

vB = vO + (! ⇥ rB/O)

B’

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+ =

Rolling Disk (no slip)

translation in x-direction

pure rotation about center

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EN40  Dynamics  and  Vibra2onsProject  #  3

 A  Trifilar  Pendulum  to  Measure  Mass  Moments  of  Iner2a  

•  What  is  a  Trifilar  Pendulum?

•  A  plaForm  hanging  by  3  cables  that  can  support  an  “object”•  If  we  perturb  the  pendulum  by  a  small  angle,  it  will  oscillate  (spin)  at  a  certain  frequency•  The  frequency  depends  on  the  mass  moment  of  inter2a

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  (i)  Derive  the  formula  that  relates  the  vibra2on  frequency  to  the  mass  moment  of  iner2a

  (ii)  Design  the  pendulum  (choose  the  dimensions,  geometry,  mass,  etc)

  (iii)  Construct  the  pendulum   (iv)  Test  the  accuracy  of  the  design   (v)  Use  the  device  to  measure  the  mass  moment  

of  iner2a  of  several  objects  of  complex  shapes  

Your  Tasks:

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Project  Schedule

• April  9  (TODAY!):  Start  analysis  of  Trifilar  Pendulum  (part  of  HW7)  • April  9:  Form  teams  of  three  students  or  fewer• April  12:  Submit  HW7  (KEEP  A  COPY)  • Week  of  April  15:  ConstrucNon  and  tesNng  • April  19:  Final  design  tesNng;  report  due.  

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•M  is  the  net  moment  of  all  forces  about  the  center  of  mass• α    is  the  angular  accelera2on• I  is  the  measure  of  the  resistance  of  the  object  to  angular  accelera2on.  It  plays  the  role  of  “mass”  in  angular  mo2on.  

New  Equa2on:        M  =  I  α

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• For  a  rigid  body,  measuring  I  is  as  important  as  measuring  its  mass!

• I  depends  on  the  mass  and  shape  of  the  body.  Can  be  easily  calculated  for  simple  geometries  (sphere,  prism,  etc.)  of  uniform  density

• Complex  geometries:  easier  to  measure!

I=mass  moment  of  iner2a

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• In  HW  #  7,  you  will  find  rota2onal  Equa2on  of  Mo2on:  

             where  L  is  the  cable  length,  m  is  the  total  mass,  R  is  the  distance  from  the  COM  to  one  of  the  cable  support  points,  I  is  the  total  mass  moment  of  iner2a.

• The  plaForm  is  given  a  small  ini2al  rota2on  and  released.  The  plaForm  oscillates;  measure  period  of  oscilla2on  to  find  total  I  

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I_TOTAL  =  I_PLATFORM  +  I_OBJECT

Measure  I_PLATFORM  with  an  “empty”  pendulum.

Load  pendulum  with  an  object  (align  CGs)

Measure  I_TOTAL,  calculate  I_OBJECT

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Design  Considera2ons

• You  must  make  sure  you  can  measure  the  period  of  the  system  sufficiently  accurately.    Eg.  Make  sure  that  you  don’t  need  to  measure  the  ;me  period  with  0.0001s  accuracy  in  order  to  measure  the  moment  of  iner;a  (MOI).  You  should  be  able  to  use  a  stop  watch  and  get  sufficient  accuracy.

• You  must  make  the  device  sensi;ve  to  the  object  of  interest.  For  example,  the  ;me  period  should  be  sufficiently  different  with  and  without  the  object,  so  that  you  can  accurately  dis;nguish  between  IplaForm  and  IplaForm+Iobject.  

• Addi;onal  design  considera;ons:     (i)  Accuracy  of  alignment  of  CM,  for  both  plaNorm  and  objects  of  

  interest.     (ii)  Mass  and  size  range  of  objects  to  study     (iii)  Support  of  various  shapes     (iv)  Robustness  of  design• Your  en;re  device  will  include  the  cables  and  a  top  support  structure.  During  tes;ng,  this  support  structure  will  be  clamped  to  another  fixed  plaNorm  in  Prince  Lab.

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Constraints• The  plaForm  must  hang  no  more  than  1.5  meters  below  its  support.  • During  the  final  tes2ng,  the  suppor2ng  structure  will  be  aeached  to  a  fixed  

structure  in  Prince  Lab  using  c-­‐clamps.  You  will  be  given  2mers  and  objects  and  told  their  masses.  You  will  then  place  an  object  in  your  device  and  demonstrate  its  use,  measuring  the  period  of  your  pendulum  in  ac2on.  You  will  be  asked  to  immediately  report  the  moment  of  iner2a  in  SI  units  based  on  this  measured  period.  No  major  adjustments  or  reconfigura2on  of  the  pendulum  will  be  permieed  during  the  tes2ng.  You  will  be  able  to  use  a  calculator  or  laptop.  

• For  preliminary  tes2ng  of  your  device,  we  suggest  that  you  weigh  and  measure  some  regularly  shaped,  uniform  objects  (disks,  blocks,  rods)  and  look  up  or  calculate  their  moments  of  iner2a.  Compare  the  known  moments  of  iner2a  with  those  found  using  your  pendulum.

• A  sample  of  poten2al  test  objects:  1.  A  bicycle  wheel  5-­‐gear  cluster  has  a  mass  of  about  412g  and  diameter  of  ~11.5  

cm  2.  A  typical  solball  has  a  mass  of  about  160g  and  a  diameter  of  ~9  cm  3.  A  football  has  a  mass  of  about  420  g  and  its  mid-­‐sec2on  diameter  is  about  16  

cm.

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Materials  and  Construc;on

• The  pendulum  may  be  constructed  from  the  following  materials:  – Foam-­‐core  board  – Perforated  Aluminum  Sheet  – Plywood  (12”x12”  squares  of  1/2”,  ¼”  thickness  should  be  available)  – 2x4

• The  top  support  structure  can  be  made  of  wood  –  plywood  is  probably  preferable.  

• Various  types  of  string  and  cable,  hooks,  bolts,  screws,  brackets,  and  other  miscellaneous  hardware  will  be  available  in  Prince  Lab.  

• Construc;on  will  take  place  in  Prince  Lab.  Hand  tools,  X-­‐Acto  knives,  and  small  power  tools  will  be  available  for  cubng  and  drilling.  

• Power  tools  may  only  be  used  under  the  supervision  of  Mr.  Brian  Corkum  or  one  of  the  Lab  TAs.  

• Mr.  Corkum  will  supervise  the  overall  use  of  the  lab,  and  is  an  invaluable  source  of  insight  and  advice.

• Construc;on  can  be  performed  during  day;me  hours  April  16-­‐20.  TAs  and  faculty  will  be  available  during  normal  sec;on  ;mes,  in  the  adernoon  hours

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Safety

• Wear  safety  glasses  when  working  on  the  project.  

• Tie  back  all  hair  and  loose  clothing.  • Clamp  all  work  pieces  while  being  cut  or  drilled  • NO  OPEN  TOED  SHOES  IN  PRINCE  LAB  • BE  CAREFUL!  

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• Classroom  sec;ons  will  not  be  held:  faculty  will  be  in  Prince  Lab!

• Evening  TA  office  hrs  will  not  be  held  next  week,  instead  TAs  are  available  during  day  for  construc;on  help!

• No  regular  faculty  office  hours,  faculty  will  be  helping  in  prince  lab  instead.

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