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Prototype	
  Test	
  	
  
○  Test	
  Conditions:	
  
■  3mm	
  HDPE	
  spheres	
  in	
  isopropyl	
  alcohol	
  solution	
  to	
  
simulate	
  sinking	
  speed	
  of	
  plankton	
  
○  Results:	
  
■  Fully	
  automated	
  control	
  
■  Steady-­‐state	
  error	
  less	
  than	
  0.1	
  mm	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  10:	
  Position	
  vs	
  Time	
  Plot	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  11:	
  Processed	
  Images	
  of	
  Controlled	
  Object	
  
FLUIDIC	
  TREADMILL	
  SYSTEM	
  
Damien	
  Blake,	
  Lingjie	
  Kong,	
  Yuling	
  Shen,	
  Yue	
  Teng	
  
Department	
  of	
  Mechanical	
  and	
  Aerospace	
  Engineering	
  at	
  University	
  of	
  California,	
  San	
  Diego	
  
Sponsored	
  by	
  Dr.	
  Jules	
  S.	
  Jaffe,	
  Dr.	
  Peter	
  Franks,	
  and	
  the	
  Scripps	
  Institution	
  of	
  Oceanography	
  
Overview	
  
	
  	
  
●  Langer	
  BT100-­‐2J	
  Peristaltic	
  Pump	
  
○  Avg.	
  flow	
  velocity	
  ranging	
  from	
  0-­‐2.8	
  mm/s	
  
○  Reads	
  external	
  signals	
  to	
  control	
  velocity	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  4:	
  Peristaltic	
  Pump	
  
	
  
●  Logitech	
  2.0	
  web	
  camera	
  and	
  lighting	
  
○  Resolution	
  of	
  5	
  µm/pixel	
  and	
  frame	
  rate	
  of	
  
30	
  	
  fps	
  
○  Compatible	
  with	
  OpenCV	
  image	
  processing	
  
software	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  5:	
  Logitech	
  2.0	
  Camera	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  1:	
  Fluidic	
  Treadmill	
  System	
  
Setup	
  
We	
   would	
   like	
   to	
   thank	
   the	
   following	
   people	
   for	
   their	
   help	
   and	
  
exper4se:	
  
●  Dr.	
  Jules	
  S.	
  Jaffe	
  and	
  Dr.	
  Peter	
  Franks	
  at	
  the	
  Scripps	
  Ins4tu4on	
  of	
  
Oceanography	
  for	
  sponsoring	
  the	
  project	
  
●  Dr.	
   Jerry	
   Tustaniwskyj,	
   Dr.	
   James	
   Babcock,	
   Michael	
   Ix	
   for	
  
guidance	
  and	
  sugges4ons	
  	
  
●  Dr.	
  Steve	
  Roberts	
  for	
  technical	
  support	
  on	
  RS-­‐485	
  interface	
  
●  Ben	
  Laxton	
  for	
  help	
  with	
  the	
  image	
  processing	
  soPware	
  	
  
●  Jessica	
  Garwood	
  for	
  guidance	
  and	
  providing	
  organism	
  samples	
  
●  Tom	
  Chalfant,	
  Ian	
  Richardson,	
  Chris	
  Cassidy	
  for	
  components	
  
●  J.V.	
  Agnew	
  for	
  purchasing	
  and	
  reimbursment	
  assistance	
  
●  Maryam	
  Sarkoush	
  for	
  ACMS	
  machine	
  access	
  
1.  Ploug,	
  Helle,	
  and	
  Bo	
  Barker	
  Jorgensen.	
  “A	
  Net-­‐jet	
  Flow	
  System	
  for	
  Mass	
  Transfer	
  and	
  Microsensor	
  Studies	
  
of	
  Sinking	
  Aggregates.”	
  
2.  Batchelor,	
  G.K.	
  (1967).	
  An	
  Introduction	
  to	
  Fluid	
  Dynamics.	
  Cambridge	
  University	
  Press.	
  ISBN	
  0-­‐521-­‐66396-­‐2	
  
3.  Lennart	
  Thomas	
  Bach,	
  Ulf	
  Riebesell,	
  Scarlett	
  Sett,	
  Sarah	
  Febiri,	
  Paul	
  Rzepka,	
  Kai	
  	
  	
  	
  	
  Georg	
  Schulz.	
  “An	
  
approach	
  for	
  particle	
  sinking	
  velocity	
  measurements	
  in	
  the	
  3–400	
  μm	
  size	
  range	
  and	
  considerations	
  on	
  the	
  
effect	
  of	
  temperature	
  on	
  sinking	
  rates”.	
  Mar	
  Biol.	
  2012;	
  159(8):	
  1853–1864.	
  Published	
  online	
  2012	
  May	
  22	
  
4.  Herndl,	
  Gerhard	
  J.	
  "Microbial	
  Control	
  of	
  the	
  Dark	
  End	
  of	
  the	
  Biological	
  Pump."	
  Nature.com.	
  Nature	
  
Publishing	
  Group,	
  29	
  Aug.	
  2013.	
  Web.	
  28	
  Apr.	
  2015.	
  
	
  
Recommendation	
   Justification	
  
Integrate	
  the	
  image	
  processing	
  
software	
  and	
  the	
  pump	
  control	
  
program	
  into	
  single	
  program	
  
Pump	
  control	
  code	
  can	
  be	
  written	
  in	
  
C++	
  using	
  an	
  open	
  source	
  library	
  
Modify	
  the	
  image	
  processing	
  code	
  
to	
  enable	
  tracking	
  of	
  the	
  object	
  
Can	
  control	
  a	
  single	
  object	
  among	
  a	
  
cluster	
  of	
  objects	
  
•  Simulation	
  of	
  Flow	
  Profile	
  
○  COMSOL	
  3D	
  Multiphysics	
  
○  Assumptions:	
  
■  Water	
  (density	
  1	
  kg	
  /	
  m3)	
  
■  No	
  Slip	
  Boundary	
  Condition	
  
■  Constant	
  Pressure	
  at	
  outlet	
  
■  Incompressible	
  Flow	
  
○  Results:	
  
■  <	
  5%	
  velocity	
  gradient	
  up	
  to	
  1.5mm	
  from	
  center	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  8:	
  Simulated	
  Flow	
  Profile	
  of	
  Chamber	
  at	
  40	
  mm	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  9:	
  Actual	
  Flow	
  Profile	
  Using	
  TiO2	
  Powder	
  Tracer	
  
	
  
1	
  
The	
   primary	
   purpose	
   of	
   the	
   fluidic	
   treadmill	
  
system	
   was	
   to	
   observe	
   the	
   sinking	
   velocities	
   of	
  
ocean	
  microorganisms,	
  such	
  as	
  phytoplankton,	
  in	
  
order	
   to	
   assess	
   their	
   carbon	
   isolation	
   properties.	
  
This	
   was	
   accomplished	
   using	
   image	
   processing	
  
and	
   flow	
   speed	
   feedback	
   control.	
   By	
   keeping	
  
them	
  in	
  the	
  field	
  of	
  view	
  of	
  a	
  camera,	
  this	
  iteration	
  
of	
   the	
   system	
   was	
   capable	
   of	
   controlling	
   test	
  
objects	
   0.5	
   mm	
   to	
   3mm	
   in	
   diameter	
   and	
  
determining	
   their	
   respective	
   sinking	
   velocities	
  
within	
  an	
  error	
  of	
  2.7	
  to	
  15.4%,	
  up	
  to	
  a	
  maximum	
  
speed	
   of	
   5.04	
   mm/s	
   .	
   With	
   future	
   improvement,	
  
the	
  fluidic	
  treadmill	
  system	
  will	
  be	
  able	
  to	
  analyze	
  
objects	
  and	
  organisms	
  to	
  a	
  size	
  of	
  50	
  μm.	
  
	
  
●  Plankton	
  and	
  other	
  microorganisms	
  in	
  the	
  ocean	
  absorb	
  
CO2	
   that	
   has	
   been	
   absorbed	
   by	
   the	
   water	
   in	
   the	
   ocean.	
  
This	
  is	
  productive	
  in	
  counteracting	
  rising	
  CO2	
  levels	
  and	
  
global	
  warming.	
  	
  
●  If	
   the	
   plankton	
   are	
   consumed	
   by	
   bacteria	
   or	
   larger	
  
organisms,	
  then	
  the	
  CO2	
  is	
  released.	
  10%	
  of	
  the	
  carbon	
  
level	
  near	
  the	
  ocean	
  surface	
  is	
  exported.	
  
●  Plankton	
   that	
   sink	
   to	
   the	
   bottom	
   of	
   the	
   ocean	
   before	
  
they	
  are	
  eaten	
  are	
  far	
  more	
  productive	
  in	
  CO2	
  isolation.	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  	
  	
  	
  	
  	
  	
  4.	
  	
  	
  	
  	
  	
  
	
  
	
  
	
  
Figure	
  12:	
  Plankton	
  Role	
  in	
  Carbon	
  Isolation	
  
●  Image	
  Processing	
  
○  C++	
  and	
  OpenCV	
  library	
  
○  Detects	
  the	
  displacement	
  between	
  observed	
  
object	
  and	
  reference	
  position	
  using	
  blob	
  
analysis	
  with	
  bounding	
  box	
  
○  Outputs	
  the	
  displacement	
  signal	
  for	
  flow	
  
velocity	
  control	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  2:	
  Image	
  Processing	
  
	
  
●  Pump	
  Flow	
  Velocity	
  Control	
  Algorithm	
  
○  MATLAB	
  and	
  RS-­‐485	
  serial	
  communication	
  
○  Based	
  on	
  the	
  displacement	
  signal	
  with	
  a	
  PI	
  
controller	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  3:	
  Feedback	
  Control	
  Block	
  Diagram	
  
	
  
●  Observation	
  chamber	
  	
  
○  Insertion	
  of	
  objects	
  through	
  quick	
  disconnect	
  
○  Allows	
  backside	
  illumination	
  and	
  imaging	
  of	
  
the	
  object	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  6:	
  Chamber	
  Setup	
  
	
  
●  Honeycomb	
  diffuser	
  	
  
○  Laser-­‐cut	
  acrylic	
  
○  9x9	
  array	
  of	
  0.75	
  mm	
  holes	
  with	
  1mm	
  pitch	
  
○  Provides	
  uniform	
  laminar	
  flow	
  profile	
  
	
  
	
  
	
  
	
  
	
  
	
  
	
  
Figure	
  7:	
  Honeycomb	
  Diffuser	
  
	
  
●  Water	
  reservoir	
  
○  Water	
  flow	
  and	
  storage	
  
○  Releases	
  air	
  bubbles	
  from	
  the	
  chamber	
  
	
  
Entering	
  field	
  of	
  view	
   Pump	
  reacting	
   Staying	
  in	
  field	
  of	
  view	
  
Timeline	
  
1	
  second	
   2	
  seconds	
   Steady	
  State	
  
Object	
  	
  
Water	
  
Reservoir	
  
Logitech	
  2.0	
  
Camera	
  
Fluidic	
  
Chamber	
  
LED	
  
Lighting	
  
Peristaltic	
  
Pump	
  
Flow	
  Profile	
  
	
  
	
  Summary	
  of	
  Performance	
  
	
  
	
  
	
  Future	
  Improvement	
  
	
  
	
  
	
  Impact	
  on	
  Society	
  
	
  
	
  
	
  Acknowledgments	
  	
  
	
  
	
  
	
  References	
  	
  
	
  
	
  So$ware	
  Components	
  
	
  
	
  
Accuracy	
  and	
  Precision	
  
	
  Distance	
  from	
  Centerline	
   Total	
  Maximum	
  Error	
  %	
  
0	
  mm	
   2.71	
  
0	
  to	
  1.5	
  mm	
   5.68	
  
1.5	
  to	
  2	
  mm	
   15.24	
  
>2.5	
  mm	
   >29	
  
	
  
	
  Hardware	
  Components	
  
	
  
Height	
  
Adjustment	
  
Quick	
  
disconnect	
  
shutoff	
  valve	
  
Honeycomb	
  
Diffuser	
  at	
  
30mm	
  
Bounding	
  
Box	
  

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Final Poster3

  • 1. Prototype  Test     ○  Test  Conditions:   ■  3mm  HDPE  spheres  in  isopropyl  alcohol  solution  to   simulate  sinking  speed  of  plankton   ○  Results:   ■  Fully  automated  control   ■  Steady-­‐state  error  less  than  0.1  mm                         Figure  10:  Position  vs  Time  Plot                   Figure  11:  Processed  Images  of  Controlled  Object   FLUIDIC  TREADMILL  SYSTEM   Damien  Blake,  Lingjie  Kong,  Yuling  Shen,  Yue  Teng   Department  of  Mechanical  and  Aerospace  Engineering  at  University  of  California,  San  Diego   Sponsored  by  Dr.  Jules  S.  Jaffe,  Dr.  Peter  Franks,  and  the  Scripps  Institution  of  Oceanography   Overview       ●  Langer  BT100-­‐2J  Peristaltic  Pump   ○  Avg.  flow  velocity  ranging  from  0-­‐2.8  mm/s   ○  Reads  external  signals  to  control  velocity                     Figure  4:  Peristaltic  Pump     ●  Logitech  2.0  web  camera  and  lighting   ○  Resolution  of  5  µm/pixel  and  frame  rate  of   30    fps   ○  Compatible  with  OpenCV  image  processing   software                     Figure  5:  Logitech  2.0  Camera                     Figure  1:  Fluidic  Treadmill  System   Setup   We   would   like   to   thank   the   following   people   for   their   help   and   exper4se:   ●  Dr.  Jules  S.  Jaffe  and  Dr.  Peter  Franks  at  the  Scripps  Ins4tu4on  of   Oceanography  for  sponsoring  the  project   ●  Dr.   Jerry   Tustaniwskyj,   Dr.   James   Babcock,   Michael   Ix   for   guidance  and  sugges4ons     ●  Dr.  Steve  Roberts  for  technical  support  on  RS-­‐485  interface   ●  Ben  Laxton  for  help  with  the  image  processing  soPware     ●  Jessica  Garwood  for  guidance  and  providing  organism  samples   ●  Tom  Chalfant,  Ian  Richardson,  Chris  Cassidy  for  components   ●  J.V.  Agnew  for  purchasing  and  reimbursment  assistance   ●  Maryam  Sarkoush  for  ACMS  machine  access   1.  Ploug,  Helle,  and  Bo  Barker  Jorgensen.  “A  Net-­‐jet  Flow  System  for  Mass  Transfer  and  Microsensor  Studies   of  Sinking  Aggregates.”   2.  Batchelor,  G.K.  (1967).  An  Introduction  to  Fluid  Dynamics.  Cambridge  University  Press.  ISBN  0-­‐521-­‐66396-­‐2   3.  Lennart  Thomas  Bach,  Ulf  Riebesell,  Scarlett  Sett,  Sarah  Febiri,  Paul  Rzepka,  Kai          Georg  Schulz.  “An   approach  for  particle  sinking  velocity  measurements  in  the  3–400  μm  size  range  and  considerations  on  the   effect  of  temperature  on  sinking  rates”.  Mar  Biol.  2012;  159(8):  1853–1864.  Published  online  2012  May  22   4.  Herndl,  Gerhard  J.  "Microbial  Control  of  the  Dark  End  of  the  Biological  Pump."  Nature.com.  Nature   Publishing  Group,  29  Aug.  2013.  Web.  28  Apr.  2015.     Recommendation   Justification   Integrate  the  image  processing   software  and  the  pump  control   program  into  single  program   Pump  control  code  can  be  written  in   C++  using  an  open  source  library   Modify  the  image  processing  code   to  enable  tracking  of  the  object   Can  control  a  single  object  among  a   cluster  of  objects   •  Simulation  of  Flow  Profile   ○  COMSOL  3D  Multiphysics   ○  Assumptions:   ■  Water  (density  1  kg  /  m3)   ■  No  Slip  Boundary  Condition   ■  Constant  Pressure  at  outlet   ■  Incompressible  Flow   ○  Results:   ■  <  5%  velocity  gradient  up  to  1.5mm  from  center                         Figure  8:  Simulated  Flow  Profile  of  Chamber  at  40  mm                     Figure  9:  Actual  Flow  Profile  Using  TiO2  Powder  Tracer     1   The   primary   purpose   of   the   fluidic   treadmill   system   was   to   observe   the   sinking   velocities   of   ocean  microorganisms,  such  as  phytoplankton,  in   order   to   assess   their   carbon   isolation   properties.   This   was   accomplished   using   image   processing   and   flow   speed   feedback   control.   By   keeping   them  in  the  field  of  view  of  a  camera,  this  iteration   of   the   system   was   capable   of   controlling   test   objects   0.5   mm   to   3mm   in   diameter   and   determining   their   respective   sinking   velocities   within  an  error  of  2.7  to  15.4%,  up  to  a  maximum   speed   of   5.04   mm/s   .   With   future   improvement,   the  fluidic  treadmill  system  will  be  able  to  analyze   objects  and  organisms  to  a  size  of  50  μm.     ●  Plankton  and  other  microorganisms  in  the  ocean  absorb   CO2   that   has   been   absorbed   by   the   water   in   the   ocean.   This  is  productive  in  counteracting  rising  CO2  levels  and   global  warming.     ●  If   the   plankton   are   consumed   by   bacteria   or   larger   organisms,  then  the  CO2  is  released.  10%  of  the  carbon   level  near  the  ocean  surface  is  exported.   ●  Plankton   that   sink   to   the   bottom   of   the   ocean   before   they  are  eaten  are  far  more  productive  in  CO2  isolation.                              4.                   Figure  12:  Plankton  Role  in  Carbon  Isolation   ●  Image  Processing   ○  C++  and  OpenCV  library   ○  Detects  the  displacement  between  observed   object  and  reference  position  using  blob   analysis  with  bounding  box   ○  Outputs  the  displacement  signal  for  flow   velocity  control                   Figure  2:  Image  Processing     ●  Pump  Flow  Velocity  Control  Algorithm   ○  MATLAB  and  RS-­‐485  serial  communication   ○  Based  on  the  displacement  signal  with  a  PI   controller               Figure  3:  Feedback  Control  Block  Diagram     ●  Observation  chamber     ○  Insertion  of  objects  through  quick  disconnect   ○  Allows  backside  illumination  and  imaging  of   the  object                         Figure  6:  Chamber  Setup     ●  Honeycomb  diffuser     ○  Laser-­‐cut  acrylic   ○  9x9  array  of  0.75  mm  holes  with  1mm  pitch   ○  Provides  uniform  laminar  flow  profile                 Figure  7:  Honeycomb  Diffuser     ●  Water  reservoir   ○  Water  flow  and  storage   ○  Releases  air  bubbles  from  the  chamber     Entering  field  of  view   Pump  reacting   Staying  in  field  of  view   Timeline   1  second   2  seconds   Steady  State   Object     Water   Reservoir   Logitech  2.0   Camera   Fluidic   Chamber   LED   Lighting   Peristaltic   Pump   Flow  Profile      Summary  of  Performance        Future  Improvement        Impact  on  Society        Acknowledgments          References        So$ware  Components       Accuracy  and  Precision    Distance  from  Centerline   Total  Maximum  Error  %   0  mm   2.71   0  to  1.5  mm   5.68   1.5  to  2  mm   15.24   >2.5  mm   >29      Hardware  Components     Height   Adjustment   Quick   disconnect   shutoff  valve   Honeycomb   Diffuser  at   30mm   Bounding   Box