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DYNAMIC MECHANICAL ANALYZER (DMA)<br />BY<br />DAVID SEHGAL <br />
  What is DMA?<br /><ul><li>DMA is a measuring instrument which is used to determine the dynamic characteristics of materi...
It applies a dynamic oscillating force to a sample and analyze the material’s response to that cyclic force.
Basically, DMA determines changes in sample properties resulting from changes in five experimental variables: temperature,...
Upper part of DMA<br />DMA+450 MODEL<br />
  How does DMA work?<br /><ul><li>The basic principle of this instrument is to exert a dynamic excitation of known amplitu...
The measurement of strains and dynamic forces yields the specimen's stiffness.
From the known geometry, one can derive mechanical properties of the material, such as modulus and loss factor or damping.
The presence of the thermal chamber allows us to perform test at different temperatures and thus determining materials' gl...
Mechanical testing<br />
Configuration of specimen and   specimen holder for different tests in DMA<br />Contd……<br />
Tension jaws for film<br />Tension jaws for bars<br />Compression plates<br />Tension jaws for bars<br />Plane shear for f...
Theoretical basis for DMA <br />Viscoelasticity :-<br />Viscoelastic materials exhibit characteristics of both viscous and...
Continued….<br />       sinusoidally applied stress<br />       measured strain<br />  phase lag between applied str...
Ratio of applied stress to measured strain</li></ul>           E* =E’ + iE” = SQRT(E’2+ E”2)<br /><ul><li>Storage modulus ...
Energy stored elastically during deformation
 “Elastic” of “viscoelastic”
 E’= E* cos
Loss modulus (E’’)
Energy loss during  deformation
“Visco” of “viscoelastic”
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Dynamic Mechanical Analyzer

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Transcript of "Dynamic Mechanical Analyzer"

  1. 1. DYNAMIC MECHANICAL ANALYZER (DMA)<br />BY<br />DAVID SEHGAL <br />
  2. 2. What is DMA?<br /><ul><li>DMA is a measuring instrument which is used to determine the dynamic characteristics of materials.
  3. 3. It applies a dynamic oscillating force to a sample and analyze the material’s response to that cyclic force.
  4. 4. Basically, DMA determines changes in sample properties resulting from changes in five experimental variables: temperature, time, frequency, force, and strain.</li></li></ul><li>Construction of DMA<br />Movable frame (main unit)<br />Fixed frame or base<br />Temperature control<br />DMA+450 MODEL<br />
  5. 5. Upper part of DMA<br />DMA+450 MODEL<br />
  6. 6. How does DMA work?<br /><ul><li>The basic principle of this instrument is to exert a dynamic excitation of known amplitude and frequency to a specimen of known dimensions.
  7. 7. The measurement of strains and dynamic forces yields the specimen's stiffness.
  8. 8. From the known geometry, one can derive mechanical properties of the material, such as modulus and loss factor or damping.
  9. 9. The presence of the thermal chamber allows us to perform test at different temperatures and thus determining materials' glass transition temperature.</li></li></ul><li> Which materials can be analyzed with DMA?<br />DMA instrument can be used to characterize mechanical and/or thermal properties of a great numbers of materials:<br />Polymers<br />Elastomers<br />Composites<br />Metals and metallic alloys<br />Ceramics, glass<br />Adhesives<br />Bitumen (solid and pasty)<br />Paint and varnish (gels or films)<br />Cosmetics (gels, spray….)<br />Oils<br />Biomaterials <br />Leather, skin hair….<br />
  10. 10. Mechanical testing<br />
  11. 11. Configuration of specimen and specimen holder for different tests in DMA<br />Contd……<br />
  12. 12. Tension jaws for film<br />Tension jaws for bars<br />Compression plates<br />Tension jaws for bars<br />Plane shear for films<br />Plane shear<br />Shear for liquid<br />Shear for pasty material<br />Dual cantilever <br />Three point bending<br />DMA+450 MODEL<br />
  13. 13. Theoretical basis for DMA <br />Viscoelasticity :-<br />Viscoelastic materials exhibit characteristics of both viscous and elastic materials<br />Ex.- Elastomers, polymers etc. <br />Viscosity  resistance to flow (damping)<br />Elasticity  ability to revert back to original shape<br /> Elastic vs viscoelastic response <br />Glass Transition Temperature (Tg)<br />Definition: Transition from bond stretching to long range molecular motion<br />Flow Temperature<br />Definition: point at which heat vibration is enough to break bonds in crystal lattice<br />
  14. 14. Continued….<br />  sinusoidally applied stress<br />  measured strain<br />  phase lag between applied stress and measured strain<br /><ul><li>Complex dynamic modulus (E*)
  15. 15. Ratio of applied stress to measured strain</li></ul> E* =E’ + iE” = SQRT(E’2+ E”2)<br /><ul><li>Storage modulus (E’)
  16. 16. Energy stored elastically during deformation
  17. 17. “Elastic” of “viscoelastic”
  18. 18. E’= E* cos
  19. 19. Loss modulus (E’’)
  20. 20. Energy loss during deformation
  21. 21. “Visco” of “viscoelastic”
  22. 22. E” = E* sin 
  23. 23. Loss tangent (tan ) or damping or loss factor
  24. 24. shows the ability of material to dissipate the energy
  25. 25. Tan = E’’/E’</li></ul> <br />
  26. 26. Continued….<br /><ul><li>If phase lag  is zero</li></ul> then E*= E’  material is purely elastic<br /><ul><li>If phase lag  is 90 degree</li></ul> then E* = E”  material is purely viscous<br /><ul><li>If phase lag  is between 0  90 degree</li></ul> then E* =E’ + iE”  material is viscoelastic<br />
  27. 27. Working of DMA<br />Contd……<br />
  28. 28. 1. Preparation of specimen<br /><ul><li>Depending on the material to analyze, the specimen can be prepared in different ways: Molding, Cutting
  29. 29. As a general rule, common specimen dimensions range from a few millimeters to a few centimeters. The use of a caliper is then advised. The use of a micrometer is preferred to measure film thickness.</li></ul>Cutting <br />Venire caliper<br />micrometer<br />
  30. 30. 2. Selection of specimen holder<br /> On the basis of<br /> - The nature of the material<br /> - specimen shape<br />DMA+450 MODEL<br />Correspondence between specimen holder and material of specimen<br />Materials specimen holder<br />Elastromer (cylinder or bar) compression plates, plane shear<br />Elastomer (band) tension jaws for bars, tension jaws for films, <br /> shear jaws for films<br />Polymer compression plates, tension jaws for bars, three <br /> point bending, dual cantilever bending, <br /> plane shear, shear jaws for films <br />Polymers (films) tension jaws for films, shear jaws for films <br />Polymers (fibers) tension jaws for fibers<br />Pasty bitumen shear for pasty material, shear for liquid materials<br />Metals, metallic alloys, ceramics three point bending, dual cantilever bending<br />
  31. 31. Continued…..<br />Correspondence between specimen holder and specimen shape<br />DMA+450 MODEL<br />
  32. 32. 3. Installation of the selected specimen holder<br />4. Installation of the prepared specimen into the specimen holder inside thermal chamber<br />5. Start temperature, finish temperature, and step<br />6. Application of dynamic excitation (stress or strain) on the specimen by dynamic shaker through entire temperature range<br />7. Then DMA records the response of specimen and<br /> determines: E’, E”, Tan<br />8. Identify transition temperatures based on noticeable changes in curves<br />
  33. 33. Result <br />DMA Graph<br /><ul><li>Storage modulus (E’):elastic property
  34. 34. Loss modulus (E”) :viscous property
  35. 35. Loss tangent (tan )
  36. 36. A typical response from a DMA shows both modulus and Tanδ. As the material goes through its glass transition, the modulus reduces and the Tanδ goes through a peak.
  37. 37. Tg indicated by major change in curves: Large drop in log E’ curve and Peak in Tanδ curve</li></li></ul><li> Testing of elastomer by DMA <br />Specimen material <br /> Elastomer <br />Specimen shape <br /> Bar<br />Test <br /> Compression test<br />Specimen holder<br /> Compression plates<br />
  38. 38. Glass transition temperature<br />
  39. 39. Thank you<br />
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