# TENSILE TESTS (ASTM D 638, ISO

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1 MODULE 4 The mechanical properties, among all the properties of plastic materials, are often the most important properties because virtually all service conditions and the majority of end-use applications involve some degree of mechanical loading. Nevertheless, these properties are the least understood by most design engineers. The material selection for a variety of applications is quite often based on mechanical properties such as tensile strength, modulus, elongation, and impact strength. The basic understanding of stress strain behavior of plastic materials is of utmost importance to design engineers. One such typical stress strain (load-deformation) diagram is illustrated in Figure 2-1. For a better understanding of the stress strain curve, it is necessary to define a few basic terms that are associated with the stress strain diagram. Stress. The force applied to produce deformation in a unit area of a test specimen. Stress is a ratio of applied load to the original cross-sectional area expressed in lb/in.2. Strain. The ratio of the elongation to the gauge length of the test specimen, or simply stated, change in length per unit of the original length ( l/l). t is expressed as a dimensionless ratio. Elongation. The increase in the length of a test specimen produced by a tensile load. Yield Point. The fi rst point on the stress strain curve at which an increase in strain occurs without the increase in stress. Yield Strength. The stress at which a material exhibits a specifi ed limiting deviation from the proportionality of stress to strain. Unless otherwise specified, this stress will be at the yield point. Proportional Limit. The greatest stress at which a material is capable of sustaining the applied load without any deviation from proportionality of stress to strain (Hooke s Law). This is expressed in lb/in.2.

2 Modulus of Elasticity. The ratio of stress to corresponding strain below the proportional limit of a material. t is expressed in F/A, usually lb/in.2 This is also known as Young s modulus. A modulus is a measure of material s stiffness. Ultimate Strength. The maximum unit stress a material will withstand when subjected to an applied load in compression, tension, or shear. This is expressed in lb/in.2. Secant Modulus. The ratio of the total stress to corresponding strain at any specific point on the stress strain curve. t is also expressed in F/A or lb/in.2. The stress strain diagram illustrated in Figure 2-1 is typical of that obtained in tension for a constant rate of loading. However, the curves obtained from other loading conditions, such as compression or shear, are quite similar in appearance. The initial portion of the stress strain curve between points A and C is linear and it follows Hooke s law, which states that for an elastic material the stress is proportional to the strain. The point C at which the actual curve deviates from the straight line is called the proportional limit, meaning that only up to this point is stress proportional to strain. The behavior of plastic material below the proportional limit is elastic in nature and therefore the deformations are recoverable. The deformations up to point B in Figure 2-1 are relatively small and have been associated with the bending and stretching of the interatomic bonds between atoms of plastic molecules as shown in Figure 2-2a. This type of deformation is instantaneous and recoverable. There is no permanent displacement of the molecules relative to each other. The deformation that occurs beyond point C in Figure 2-1 is similar to a straightening out of a coiled portion of the molecular chains (Figure2-2b). There is no intermolecular slippage and the deformations may be recoverable ultimately, but not instantaneously. The extensions that occur beyond the yield point or the elastic limit of the material are not recoverable (Figure 2-2c). There deformations occur because of the actual displacement of the molecules with respect to each other. The displaced molecules cannot slip back to their original positions and, therefore, a permanent deformation or set occurs. These three types of deformations, as shown in Figure 2-2, do not occur separately but are superimposed on each other. The bonding and the stretching of the interatomic bonds are almost instantaneous. However, the molecular uncoiling is relatively slow. Molecular slippage effects are the slowest of all three deformations The polymeric materials can be broadly classifi ed in terms of their relative softness, brittleness, hardness, and toughness. The tensile stress strain diagrams serve as a basis for such a classifi cation (6). The area under the stress strain

3 curve is considered as the toughness of the polymeric material. Figure 2-4a illustrates typical tensile stress strain curves for several types of polymeric materials. A soft and weak material is characterized by low modulus, low yield stress, and a moderate elongation at break point. Polytetrafl uoroethylene (PTFE) is a good example of one such type of plastic material. A soft but tough material shows low modulus and low yield stress, but very high elongation and high stress at break. Polyethylene is a classic example of these types of plastics. A hard and brittle material is characterized by high modulus and low elongation. t may or may not yield before breaking. One such type of polymer is general purpose phenolic. A hard and strong material has high modulus, high yield stress, usually high ultimate strength, and low elongation. Acetal is a good example of this class of materials. A hard and tough material is characterized by high modulus, high yield stress, high elongation at break, and high ultimate strength. Polycarbonate is considered a hard and tough material. Figure 2-4b illustrates the relation between ductility and strength. TENSLE TESTS (ASTM D 638, SO 527-1) Tensile elongation and tensile modulus measurements are among the most important indications of strength in a material and are the most widely specified properties of plastic materials. Tensile test, in a broad sense, is a measurement of the ability of a material to withstand forces that tend to pull it apart and to determine to what extent the material stretches before breaking. Tensile modulus, an indication of the relative stiffness of a material, can be determined from a stress strain diagram. Different types of plastic materials are often compared on the basis of tensile strength, elongation, and tensile modulus data. Many plastics are very sensitive to the rate of straining and environmental conditions. Apparatus The tensile testing machine of a constant-rate-of-crosshead movement is used. t has a fi xed or essentially stationary member carrying one grip, and a movable member carrying a second grip. Self-aligning grips employed for holding the test specimen between the fixed member and the movable member prevent alignment problems. A controlledvelocity drive mechanism is used. Some of the commercially available machines use a closed-loop servo-controlled drive mechanism to provide a high degree of speed accuracy. Test Specimens and Conditioning Test specimens for tensile tests are prepared many different ways. Most often, they are either injection molded or compression molded. The specimens may also be prepared by machining operations from materials in sheet, plate, slab, or similar form. Test specimen dimensions vary considerably depending upon the requirements and are

4 described in detail in the ASTM book of standards. Figure 2-9 shows ASTM D 638 Type tensile test specimen most commonly used for testing rigid and semirigid plastics. The specimens are conditioned using standard conditioning procedures. Since the tensile properties of some plastics change rapidly with small changes in temperature, it is recommended that tests be conducted in the standard laboratory atmosphere of 23 } 2 C and 50 } 5 percent relative humidity. Test Procedures A. Tensile Strength The speed of testing is the relative rate of motion of the grips or test fixtures during the test. There are basically five different testing speeds specified in the ASTM D638 Standard. The most frequently employed speed of testing is 0.2 in./min. Whenever possible, the speed indicated by the specification for the material being tested should be used. f a test speed is not given, appropriate speed that causes rupture between 30 sec and 5 min should be chosen. The test specimen is positioned vertically in the grips of the testing machine. The grips are tightened evenly and firmly to prevent any slippage. The speed of testing is set at the proper rate and the machine is started. As the specimen elongates, the resistance of the specimen increases and is detected by a load cell. This load value (force) is recorded by the instrument. Some machines also record the maximum (peak) load obtained by the specimen, which can be recalled after the completion of the test. The elongation of the specimen is continued until a rupture of the specimen is observed. Load value at break is also recorded. The tensile strength at yield and at break (ultimate tensile strength) are calculated. B. Tensile Modulus and Elongation Tensile modulus and elongation values are derived from a stress strain curve. An extensometer is attached to the test specimen as shown in Figure 2-10a. The extensometer is a strain gauge type of device that magnifi es the actual stretch of the specimen considerably. Reliability of the strain measurement is affected by the traditional contact extensometers due to the actual physical contact with the test specimen. n recent years, many test equipment manufacturers have developed noncontact measurement systems based on optical, video and laser devices to overcome problems associated with contact extensometers. FLEXURAL PROPERTES (ASTM D 790, SO 178) The stress strain behavior of polymers in fl exure is of interest to a designer as well as a polymer manufacturer. Flexural strength is the ability of the material to withstand bending forces applied perpendicular to its longitudinal axis. The stresses induced by the fl exural load are a combination of compressive and tensile stresses. This effect is illustrated in Figure Flexural properties are reported are reported and calculated in terms of the maximum stress and strain that occur at the outside surface of the test bar. Many polymers do not break under fl exure even after a large defl ection that makes determination of the ultimate fl exural strength impractical for many polymers. n such cases, the common practice is to report fl exural yield strength when the maximum strain in the outer fi ber of the specimen has reached 5 percent. For polymeric materials that break easily under fl exural load, the specimen is defl ected until a rupture occurs in the outer fi bers. Figure Forces involved in bending a simple beam.

6 Mechanical Behaviour of Plastics 85 they do aid in the understanding and analysis of the behaviour of viscoelastic materials. Some of the more important models will now be considered. (a) Maxwell Model The Maxwell Model consists of a spring and dashpot in series at shown in Fig This model may be analysed as follows. Fig The Maxwell model Stress-Strain Relations The spring is the elastic component of the response and obeys the relation O'1 -- ~'E1 (2.27) where Crl and el are the stress and strain respectively and ~ is a constant. The dashpot is the viscous component of the response and in this case the stress t~2 is proportional to the rate of strain e2, ie where r/is a material constant. Equilibrium Equation For equilibrium of forces, assuming constant area Geometry of Deformation Equation ~2 = ~" k2 (2.28) Applied Stress, cr- ttl = ~2 (2.29) The total strain, e is equal to the sum of the strains in the two elements. So ~--- ~l -~" ~2 (2.30)

7 86 Mechanical Behaviour of Plastics From equations (2.27), (2.28) and (2.30) 1 1 k = 'Sbl +--0"2 r/ 1 1 k b o- (2.31) o This is the governing equation of the Maxwell Model. t is interesting to consider the response that this model predicts under three common timedependent modes of deformation. (i) Creep f a constant stress, cro, is applied then equation (2.31) becomes 1 = -.tro (2.32) r/ which indicates a constant rate of increase of strain with time. From Fig it may be seen that for the Maxwell model, the strain at any time, t, after the application of a constant stress, tro, is given by Cro e ( t ) = -( + tr~ bt d 41-- q/) llb _(To r 0 tl L L"% Relaxation 1 1 tl! t _ J i 6'='~" Recovery Z t2 - Time--- Time Fig Response of Maxwell model

8 Mechanical Behaviour of Plastics 87 Hence, the creep modulus, E(t), is given by (ii) Relaxation E(t) = = (2.33) e(t) r/4-/~t f the strain is held constant then equation (2.31) becomes 1 1 0= --&+-.or Solving this differential equation (see Appendix B) with the initial condition e = Cro at t = to then, -~t cr(t) = croe n (2.34) tr(t) =tro e-t/tr (2.35) where TR = r//~ is referred to as the relaxation time. This indicates that the stress decays exponentially with a time constant of r//~ (see Fig. 2.35). (iii) Recovery When the stress is removed there is an instantaneous recovery of the elastic strain, e, and then, as shown by equation (2.31), the strain rate is zero so that there is no further recovery (see Fig. 2.35). t can be seen therefore that although the relaxation behaviour of this model is acceptable as a first approximation to the actual materials response, it is inadequate in its prediction for creep and recovery behaviour. (b) Kelvin or Voigt Model n this model the spring and dashpot elements are connected in parallel as shown in Fig Fig The Kelvin or Voigt Model

9 88 Mechanical Behaviour of Plastics Stress-Strain Relations These are the same as the Maxwell Model and are given by equations (2.27) and (2.28). Equilibrium Equation For equilibrium of forces it can be seen that the applied load is supported jointly by the spring and the dashpot, so Geometry of Deformation Equation cr = crl + or2 (2.36) n this case the total strain is equal to the strain in each of the elements, i.e. From equations (2.27), (2.28) and (2.36) e = el = e2 (2.37) cr = ~. el + Ok2 or using equation (2.37) tr = ~. e + r/. k (2.38) This is the governing equation for the Kelvin (or Voigt) Model and it is interesting to consider its predictions for the common time dependent deformations. (i) Creep f a constant stress, %, is applied then equation (2.38) becomes ao=~.e+o~ and this differential equation may be solved for the total strain, e, to give e(t) = ~ l-e- where the ratio r//~ is referred to as the retardation time, TR. This indicates an exponential increase in strain from zero up to the value, tro/~, that the spring would have reached if the dashpot had not been present. This is shown in Fig As for the Maxwell Model, the creep modulus may be determined as oo [,], E(t) = 6(0 = ~" 1 - e-~ (2.39)

10 Mechanical Behaviour of Plastics 89 t Asymptote ~ = ao/p,... ~T... %1 _t---"",~' i "=-Creep.~" i L\ Recow, y ~ h '<i i 0 tl t2 Time Relaxation - ao 0 i! i,, 0 tl t 2 v Time Fig Response of Kelvin/Voigt model (ii) Relaxation f the strain is held constant then equation (2.38) becomes That is, the stress is constant and supported by the spring element so that the predicted response is that of an elastic material, i.e. no relaxation (see Fig. 2.37) (iii) Recovery f the stress is removed, then equation (2.38) becomes 0=~.e+o~ Solving this differential equation with the initial condition e = e' at the time of stress removal, then e(t) = e'e- ~ (2.40) This represents an exponential recovery of strain which is a reversal of the predicted creep. (c) More Complex Models t may be seen that the simple Kelvin model gives an acceptable first approximation to creep and recovery behaviour but does not account for relaxation. The Maxwell model can account for relaxation but was poor in relation to creep

11 90 Mechanical Behaviour of Plastics and recovery. t is clear therefore that some compromise may be achieved by combining the two models. Such a set-up is shown in Fig n this case the stress-strain relations are again given by equations (2.27) and (2.28). The geometry of deformation yields. Total strain, e = e~ + e2 -- ek (2.41) Fig Maxwell and Kelvin models in series where ek is the strain response of the Kelvin Model. From equations (2.27), (2.28) and (2.41). tro trot Cro[ _~gz!] g ( t ) = -~l "~" g] " + -~ e ~2 (2.42) From this the strain rate may be obtained as ~ = r b cro -~t ~- ~e,~2 (2.43) r/1 r/2 The response of this model to creep, relaxation and recovery situations is the sum of the effects described for the previous two models and is illustrated in Fig t can be seen that although the exponential responses predicted in these models are not a true representation of the complex viscoelastic response of polymeric materials, the overall picture is, for many purposes, an acceptable approximation to the actual behaviour. As more and more elements are added to the model then the simulation becomes better but the mathematics become complex. Example 2.12 An acrylic moulding material is to have its creep behaviour simulated by a four element model of the type shown in Fig f the creep curve for the acrylic at 14 MN/m 2 is as shown in Fig. 2,40, determine the values of the four constants in the model.

12 Mechanical Behaviour of Plastics 91 J Recovery ~_ ao! o -i.... tl... t2 nm~ e = ~ 2 0 Oo ~,' i... l i t~ t2.... F Time Fig Response of combined Maxwell and Kelvin models Stres~ MNm 2 C " ~ ~ / , Slope = -~ = X 10 "s hr -1 o ~oo 2oo ~o ~ Time (hours) Fig Creep curve for acrylic at 20~ Solution The spring element constant, ~1, for the Maxwell model may be obtained from the instantaneous strain, e~. Thus ~1 = O'~ = MN/m 2 el The dashpot constant, 01, for the Maxwell element is obtained from the slope of the creep curve in the steady state region (see equation (2.32)). tro 14 r/1 = ~ = = 1.2 x 107 MN.hr/m 2 e x 10-6 = 4.32 x 10 l~ MN.s/m 2

13 92 Mechanical Behaviour of Plastics The spring constant, ~2, for the Kelvin-Voigt element is obtained from the maximum retarded strain, e2, in Fig ~ o = 14 = 7000 MN/m 2 e2 ( )10-2 The dashpot constant, 0z, for the Kelvin-Voigt element may be determined by selecting a time and corresponding strain from the creep curve in a region where the retarded elasticity dominates (i.e. the knee of the curve in Fig. 2.40) and substituting into equation (2.42). f this is done then 02 = 3.7 x 108 MN.s/m 2. Having thus determined the constants for the model the strain may be predicted for any selected time or stress level assuming of course these are within the region where the model is applicable. (d) Standard Linear Solid Another model consisting of elements in series and parallel is that attributed to Zener. t is known as the Standard Linear Solid and is illustrated in Fig The governing equation may be derived as follows. Fig The standard linear solid Stress-Strain Relations As shown earlier the stress-strain relations are 0.1 ~ ~E1 0" 2 =~2E2 0"3 "-- ~3~3 (2.44) (2.45) (2.46) Equilibrium Equation n a similar manner to the previous models, equilibrium of forces yields. 0.1 "-0"3 tr = trl + a2 (2.47)

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