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4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
Non Newtonian Fluids : Oobleck
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
A b s t r a c t
A non newtonian fluid composed of a suspensi-
non of one part water to two parts corn starch is a
demonstration of a shear thickening fluid, mean-
ing the greater the amount of stress the material
undergoes the greater the viscosity increases.
Simply meaning the more force acting on
the liquid body, the more is acts as a solid.
Also known as a dilatant, this fluid’s properties are
qualified by particle size, shape, and distribution, all
ofwhicharegovernedbyforceoveranintervaloftime.
The faster the force is applied, the greater of
observable reaction. The thickening reaction
therefore relies on both a quick stress force and
significant amount of force entering the
system to act as a non newtonian fluid.
Current applications of these procedures are seen
through industries where either friction or force
is needed to inhibit or slow movement; traction
control systems and braking mechanisms, as well
as body armor applications are two such areas.
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
equilibrium thickened
acts as a liquid acts as a solid
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
material variables constant variables operated variables
viscosity viscosity
time time
force force
shape shape
particle size particle size
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
if the end goal is to manufacture shape from this material through the use of sound
intervention, how can one meaningfully test and retest reliable
geometry, form making techniques, and explore material quality?
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
three density types five sound bytes
01 04 07 10 13 02 05 08 11 14 03 06 09 12 15
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
01 02 03
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
04 05 06
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
07 08 09
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 11 12
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
13 14 15
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
to develop a drying / molding procedure for casted, fluid suspensions; with an emphasis on lessening
material usage, reducing total weight, lowering density, and enhancing the internal strengths.
design intent
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
sound particle travel
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
observed reactions
equilibrium thickened
sound wave
fluid suspension
internal thickening
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
potential ideal shape
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
rippled surface
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
parametric variables
particle size
sound wave
amplitude + frequency
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
16 18 20 22 24 17 19 21 23 25
two new suspensions
silicate based + aggregate based
five sound bytes
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
16 17
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
18 19
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
20 21
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
22 23
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
24 25
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
after analyzing various fluid suspensions, the realization that these systems of interaction could be
understood most intuitively at the particle level became apparent. which led me to conceptualizing a
weighted parametric scheme to document the extents of my observations.
parametric schema
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
parametric schema
particle thickening
waveform spectrum
amplitude [time]
frequency[hertz]
distance[meters]
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
the application of sound to non newtonian fluid suspensions, such as concrete, types of silicates, and
plasters, has the potential to yield lighter weight units by using less material than prior prototypes.
by scattering, moving, jumping, and reacting to attuned frequencies, the poured substance would
either disperse and coat the interior of a mold to create a shell or form a lattice like network that would
be bounded by the contraints of the mold.
both drying procedures would achieve a lighter weight and less dense volume. as for sturctural
integrity? that question will have to wait until next semester!
future applications
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
4.S52 | Shape and Material | Spring 2013
Eric Randall Morris
Thank You!

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EMorris_OobleckPresentation

  • 1. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris Non Newtonian Fluids : Oobleck
  • 2. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris
  • 3. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris A b s t r a c t A non newtonian fluid composed of a suspensi- non of one part water to two parts corn starch is a demonstration of a shear thickening fluid, mean- ing the greater the amount of stress the material undergoes the greater the viscosity increases. Simply meaning the more force acting on the liquid body, the more is acts as a solid. Also known as a dilatant, this fluid’s properties are qualified by particle size, shape, and distribution, all ofwhicharegovernedbyforceoveranintervaloftime. The faster the force is applied, the greater of observable reaction. The thickening reaction therefore relies on both a quick stress force and significant amount of force entering the system to act as a non newtonian fluid. Current applications of these procedures are seen through industries where either friction or force is needed to inhibit or slow movement; traction control systems and braking mechanisms, as well as body armor applications are two such areas.
  • 4. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris equilibrium thickened acts as a liquid acts as a solid
  • 5. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris material variables constant variables operated variables viscosity viscosity time time force force shape shape particle size particle size
  • 6. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris if the end goal is to manufacture shape from this material through the use of sound intervention, how can one meaningfully test and retest reliable geometry, form making techniques, and explore material quality?
  • 7. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris three density types five sound bytes 01 04 07 10 13 02 05 08 11 14 03 06 09 12 15
  • 8. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 01 02 03
  • 9. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 10. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 04 05 06
  • 11. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 12. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 07 08 09
  • 13. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 14. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 11 12
  • 15. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 16. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 13 14 15
  • 17. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 18. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris to develop a drying / molding procedure for casted, fluid suspensions; with an emphasis on lessening material usage, reducing total weight, lowering density, and enhancing the internal strengths. design intent
  • 19. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris
  • 20. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris sound particle travel
  • 21. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris
  • 22. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris observed reactions equilibrium thickened sound wave fluid suspension internal thickening
  • 23. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris
  • 24. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris potential ideal shape
  • 25. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris
  • 26. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris rippled surface
  • 27. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris
  • 28. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris parametric variables particle size sound wave amplitude + frequency
  • 29. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 16 18 20 22 24 17 19 21 23 25 two new suspensions silicate based + aggregate based five sound bytes
  • 30. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 16 17
  • 31. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 32. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 18 19
  • 33. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 34. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 20 21
  • 35. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 36. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 22 23
  • 37. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 38. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 24 25
  • 39. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris 10 seconds 20 seconds 30 seconds 40 seconds 50 seconds 60 seconds
  • 40. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris after analyzing various fluid suspensions, the realization that these systems of interaction could be understood most intuitively at the particle level became apparent. which led me to conceptualizing a weighted parametric scheme to document the extents of my observations. parametric schema
  • 41. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris parametric schema particle thickening waveform spectrum amplitude [time] frequency[hertz] distance[meters]
  • 42. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris the application of sound to non newtonian fluid suspensions, such as concrete, types of silicates, and plasters, has the potential to yield lighter weight units by using less material than prior prototypes. by scattering, moving, jumping, and reacting to attuned frequencies, the poured substance would either disperse and coat the interior of a mold to create a shell or form a lattice like network that would be bounded by the contraints of the mold. both drying procedures would achieve a lighter weight and less dense volume. as for sturctural integrity? that question will have to wait until next semester! future applications
  • 43. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris
  • 44. 4.S52 | Shape and Material | Spring 2013 Eric Randall Morris Thank You!