Creep Behaviour of Materials

specter Behaviour of MaterialsChen Yi LingObjectivesThe objectives of the experiment argonTo measure the looney aberration in strike and polypropene at room temperatureTo determine the effect of filt roam on the crazy torsion of strike and polypropyleneTo appreciate the difference in creep demeanour between these two classes of temporalsTo be aw atomic number 18 of creep as a design con fountrationTheory2.1. IntroductionDeformation under a certain applied laden over a clip period of fourth dimension at a particular temperature is define as creep, and it limits the load carrying substance among structual strongs.When subjected to a tautness greater or equal to its yield tension, the tangible deforms plastically. Alternately, when the stress is less than its yield stress, the material leave deform waxyally.However, when the material has to withstand stress at high temperature, permanent deformation impart occur even if the stress is below the yield stress obtain ed from a malleable footrace. Under a regular stress, the air vary as a function of time as facen in range of a function 2.1.1. 1The divergent stages of creep argonPrimary Creep/Transient Creep rail line localise decreases with time and deformation becomes difficult as stress increases. (i.e. mannikin Hardening)Secondary Creep/Steady CreepStrain reckon is unbrokenThe occurrence is cod to the balance between soma hardening and give softening (Structure Recovery)Tertiary Creep/Approaching RuptureStrain rate increases with time and the material is fractured.Increase in creep rate is due to the increasing number of damages such as cavities, cracks and necking.The damaging phenomena slim down the cross-sectional area, which increase the applied stress when determined under eternal load.Viscoelastic materials such as polymers and metals are susceptible to creep. When subjected to a explosive force, the response of a polymeric material can be find using the Kelvin-Voig t model (Figure 2.1.2)Viscoelastic materials experience an increase in strain with time when subjected to a eonian stress, this is termed as viscoelastic creep. At t0 (Figure 2.1.3), viscoelastic material is able to maintain for a significant long period of time when loaded with a aeonian stress. The material eventually fails when it responds to the stress with an increasing strain. In contrast, when the stress is maintained for a shorter period of time, the material experience an initial strain until t1 in which the stress is relieved. The strain indeed immediately decrease gradually to a residual strain. 3In this experiment, we will study the creep behaviour of a low-melting point metal (Lead, Pb) and a polymer (polypropene, PP) at room temperature.2.2. Creep in MetalsCreep can be observed in all metals if its operating temperature exceeds 0.3 to 0.5Tm 5 (Tm = Absolute Melting Temperature) (Figure 2.2.1)Creep strain () depends on several variables, the most beta variables are stress () and temperature (T). utilise stress and temperature, the creep rate () can be defined as ( equality 2.2.1)Where,A = Constantn = Stress ExponentE = Activation energy for creepR = Universal gas constantCreep rate () increase as stress and temperature increase, hence Equation 2.2.1 can be redefined as (Equation 2.2.2)Whereby n is the slope of vs lnA at constant temperature.2.3. Creep in PolymersThe creep in polymers is almost similar to the creep in metal as it is depends on stress and temperature, with a a few(prenominal) barions. Comparing Figure 2.2.1 and Figure 2.3.1, the two graphs look similar except that Figure 2.3.1 has a recovery phase, which is termed as the reversal of creep.Possessing viscoelastic properties, the demeanour of the material can be predicted using the Kelvin-Voigt model (Figure 2.1.2) as mentioned earlier, and hence, it will be utilise in this experiment.Equation 2.3.1 shows the relationship between the creep strain () and time under constant stress (Equation 2.3.1)Where and are the constant of the spring and dashpot respectively (Figure 2.1.2)On the other hand, Equation 2.3.2 shows the creep strain in relation to time (Equation 2.3.2)Where is a constant.The data obtained can be plotted into an isochronous graph by taking the constant time section through the creep curves for a specialized temperature. And the results obtained formed the isochronous graph. tryal Procedures3.1 Equipment for Creep TestingThe load was applied steadily to the type using the lever principle shown in Figure 3.1.1. Steel pins were used to kept the ideal in place on one side of the lever and the weight hanger on the other.The weight hanger consist of 2 immobilize position the topmost hole was used when the hanger and lade were in consist position while the depress hole was used when the hanger was loaded.The following dining table shows the mass for the parts of the equipment which should be taken into consideration during the calc ulation of tensile force on the modelIf m was the mass of the load on the weight hanger, then the tensile force acting on the exemplar can be defined by taking moment approximately pivot as shown in Figure 3.1.2.(F+0.04) x 42 0.40 x 147 (0.16 + 0.04 +m) x 336 = 0 (Equation 3.1.1)Where, g is the acceleration due to gravity = 9.807m/s2The cite of the specimen was measured using a dial gauge (DG). The DG was placed into a tube trim downed using a nylon pinch cavil to view as the DG in its place. It should be noned that the nylon pinch screw should only when be tighten sufficiently to prevent the DG from moving when the loads were placed.The top of the DG was attached to the set up using a grooved plate which was bolted to the lever build. This arrangement was to ensure the groove in this plate was two times the distance from the pivot to the centre of the specimen. Hence, the prolongation of the specimen detected by the DG was twice the genuine extension of the specimen. And to counter for inaccuracy when zeroing the DG, an additional 3mm was taken into account before the start of the experiment.Thus, the actual extension of the specimen can be calculated by (Equation 3.1.2)3.2 Experiment MethodsFor the touchstone of creep in lead, the load applied would be 0.9, 1.0 and 1.1kg. For the measurement of creep in polypropylene, the load applied would be 0.7, 0.8 and 0.9kg. originally conducting the experiment, the width, length, ponderousness and gauge length of the specimen was measured thrice using an electronic vernier caliper the denotations used for the calculation would be the average reading (highlighted in orange).3.2.1 Experiment 1 Creep of LeadThe lever arm was held in place using 2 pins 1 of it to be inserted into the tutelage block and the other onto the topmost hole of the weight hanger.Attached the specimen onto the set up using 2 pins.Place the control pretend into the hole/tube but do not tighten the nylon screw yet.Attach the gro ove plate at the top of the Dial hazard and lever arm and secure it using a thumb nut. carrier bag the pin holding the weight hanger to take up any slack movement.Make sure the specimen was placed vertically.Carefully adjust the Dial Gauge until the inner dial reads 3mm and the appearer ring reads 0, then tighten the nylon screw.Load the indispensable weight onto the hanger.Raise the loaded weight hanger to the lower hole (loading position) and insert the pin.Gently release the load and start throw overboard watch.Record reading every 15 seconds for 30 minutes or till the specimen splits.In order to determine the secondary creep rate for each applied stress, 3 extension-time creep curves were postulate. The creep rate can be calculated using the following equation (Equation 3.2.1.1)Where In this experiment, ln vs ln plot was required. Hence, the stress () on the specimen is given by (Equation 3.2.1.2)Where, F is the load applied to the specimen (N)3.2.2 Experiment 2 Creep of polypropeneThe test of creep of polypropylene is similar to that of lead, with a couple of exceptions. Before placing the specimen onto the set up, 2 U brackets should be fitted over the 2 ends of the specimen. For polypropylene, elastic recovery was possible hence the specimen was not required to be tested until failure. Note that 15 minutes, 12 minutes and 7 minutes were the extension time required for 0.6kg, 0.7kg and 0.8kg respectivelyPlace the required load onto the weight hanger.Record the extension for every 15 seconds for specific duration.After the extension period, remove the weights on the weight hanger and continue to take the reading (elastic recovery phase) every 15 seconds for 10 minutes or when the needle on the Dial Gauge stop moving for 1 minute.Repeat for other loads.Plot extension vs time curve to show the creep and recovery curve.In this experiment, strain vs stress plot was required. Hence, the strain rate () on the specimen is given by (Equation 3.2.2.1)W here ResultsResults for LeadThe outgrowth of extension () was selected based on the results reflected on Figure 4.1.1.The creep rate () of Lead was determine using Equation 3.2.1.1.The stress () applied onto the lead specimen was calculated using Equation 3.2.1.2.By adding ln to the grades of and , exploitation the data from Table 4.1.1, we can plot a linear graph. base on Figure 4.1.2, the stress exponent (n) from the straight line was 10.503.Results for PolypropyleneA sudden drop was observed for 0.7kg, this was due to human fault as results was not recorded promptly on specific time.Using Equation 3.2.1.2 3.2.2.1, the stress and strain rate is shown belowBased on Figure 4.2.1, when stress is constant, the strain increases as time increases, which tallies with the theory.5. Discussion public-service corporation of the Plot of ln vs lnBy plotting ln against ln, we can determine the gradient (n) or the stress exponent of the specimen, which correspond to the controlling mechanis m of creep under interrogatory conditions.Stress Exponent for LeadThe stress exponent indicates the influence of deformation rate on the mechanical strength of the specimen.7At low stresses, n equals to 1, which indicates pure diffusion creep. At high stresses, n 1, indicating other move mechanism besides pure diffusion.Factors affecting the stress exponent valueThe stress exponent for lead in this experiment was found out to be 10.503. And the factors which affects the value is the type of creeping mechanism behind the specimen. rough creeping mechanisms include Coble creep (Grain boundary diffusion) and Dislocation creep/ mount up (Power law creep).8Creep of Metals in Design ConsiderationThe following are some methods to minimize creeping in metalsEmploy materials with high TmReduce the effect of grain boundaries by using a mavin crystal with large grains or adding solid solutions to eliminate vacancies9Creep is an important consideration for when a component have to support a load at temperatures where Tabs/TM 0.4.10For high temperature, creep is an important consideration in these three areasDisplacement-limited applications such as turbine rotors in jet enginesRupture-limited applications such as high pressure steam pipesStress Relaxation limited applications such as tightened bolts and suspended cables 11Viscoelastic BehaviourMaterials which exhibits both viscous and elastic property during deformation is known as viscoelasticity.12 In this experiment, both lead and polypropylene exhibits viscoelasticity to different extend. For lead, the time taken in which the specimen rupture decreases as the stress increases. However, its viscoelasticity is not high hence, its recovery phase is not as significant as polypropylene. Furthermore, the organize of lead is more transparent than polypropylene, which means it is more brittle and more prone to rupture.For polypropylene, the extension increases as the stress increases. The extension and recovery rate of each load are as followRecovery rate is possible on polypropylene specimen because it has higher elasticity due to its amorphous structure. The amorphous structure untangles and lengthens out until it becomes crystalline.ConclusionIn conclusion, the results obtained from the experiment is true to theory. Unfortunately, during the creep test for lead, some results are missing due to some human erroneous belief resulting in an incomplete graph as depicted in Figure 4.2.1.For the creep in lead, load 1.0kg and 1.1kg rupture before 30 minutes. This shows that the heavier the load, the immediate the creep rate. At even high temperature, t