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The Mechanical Testing of Polymers and their Composites By Gordon Williams.

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1 The Mechanical Testing of Polymers and their Composites By Gordon Williams

2 Introduction Standard methods are vital in ensuring reliable data True in all fields – Thus ASTM & ISO If a property is to be claimed it must be backed by 1) a method and 2) statistical analysis ( means,SD) For materials science ;materials development must be supported by proper results.

3 Introduction e.g. Toughened polymers (PA,PE), Filled polymers; glass filled ;particle filled Nano Composites Recent confusion in “Nano” field is often a result of poor data.

4 Test Types A range from direct product testing to basic properties,e.g. Drop tests to Young’s Modulus. Intermediate type, Testing special plaques or bowls. Basic Tests measure material properties independent of size and method.

5 Test Types Two Main Types Deformation behaviour; to find Young’s Modulus,Yield stress,Poisson’s Ratio,Elongation*,Strength*. Fracture Behaviour; to find Toughness,K1c,Izod*, Charpy*. All use Tension, Compression or Bending Tests. * See later; not usually a good idea.

6 Testing Machines A long history e.g. 1880 Originally to test steel, e.g. Harbour Bridge Machines in Civil Eng. Dept. from 1908 All work in a similar way Load applied via a screw ( Instron) or hydraulic rams (Servo Hydraulic) Load measured by load cells (must calibrate)

7 Test machine  Instron 4302

8 Test machine  Instron 1195

9 Test machine  MTS 810

10 Testing Machines Deformations; Cross head,Gauge length? Extensometers, videos. Modern machines are speed controlled, i.e. constant or exponential. Polymers are rate dependent, i.e. are visco-elastic.

11 Deformation Properties Measured in; Tension,compression or bending. Tension; simplest but; end effects (dog bones),gripping (slipping),accurate strains difficult. Compression; no gripping problems However,friction. Necessary for some yield stress tests.

12 Definition of Deformation Strain,  Stress,  yy yy FF FF 2% 0  E

13 Illustrations of Deformation b W l   =  / l  =F/bW E =  /  = (F/  )( l /bW) Tension:

14 Illustrations of Deformation Compression:

15 Illustrations of Deformation E =  /  = (F/  )( l /bW)( l 2 /4W 2 ) Bending: b W l F 

16 Deformation Properties Bending Good for Modulus (magnification) However; variable strain, inhomogeniety (flexural modulus) Interpretation of curves. Young’s Modulus; elastic property,polymers are visco-elastic,rate dependent,unloading and hysterysis.Usually non- linear.

17 Deformation Behaviour Yield Stress; onset of permanent deformation, hard to define. 2% offset,maximum stress. “Correct” or “definable” ? Fracture stress/strain,strength.Variable (surface finish).A property? Fracture Mechanics!! See next week.

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