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1.0 Abstract
The elastic modulus, yield point, and ultimate strength of mild steel were determined in uniaxial tension. The "dogbone" specimen geometry was used with the region of minimum cross section having the dimensions: thickness =1.04 mm, width = 3.14 mm, and length section = 30 mm. This experiment was accomplished by first placing our specimens one at a time into a tensile testing machine (A G.U.N.T Hamburg Tensile Testing Machine (Max. load = 2kN)), which, under physical control, slowly increased the tension force on each specimen, stretching each until failure. We then analyzed the data output from the load and extension gauge. Referring from the resultant graph, we can see that the obtained graph line is straight until the one point it decrease gradually and be rupture. This shows that both variables on the graph are linearly related with each other. From the data obtained, we identify types of fracture surface of mild steel under tensile loading. The yield strength was determined to be 165.165MPa.The ultimate strength was determined to be 285.285MPa.Calculation for percentage elongation was determined to be 43 percent. After all, experimental result was compared with theoretical data.
Table of Contents1.0Abstract12.0Introduction43.0Objectives54.0Theory65.0Experimental Procedure85.1Apparatus/Experimental Setup85.2Procedure96.0Data107.0References168.0Appendices17
List of table:Table 1: Data13
List of Figures:Figure 1: Standard tensile test specimen4Figure 2: Sample mild steel shape6Figure 3: Stress-strain graph of mild steel7Figure 4: G.U.N.T Hamburg Tensile Testing Machine (Max. load = 2kN)8Figure 5: Specimen (aluminum)8Figure 6: Vernier calliper8Figure 7: Load(kN) vs Extension(mm) graph14Figure 8: Stress vs strain graph14
List of SymbolsA Area over which force (F) acts (m2)E Elastic modulus (GPa)F Force (N)Initial dimension in direction i (mm)T Specimen thickness (m)Rate of chart displacement (mm/min) Rate of sample displacement (mm/min)w Specimen width (m) Displacement of chart (mm) Displacement of sample (mm) Strain =0 Predicted strain at zero stress Normal strain in direction iE Error in the predicted elastic modulus (GPa)F Error in the force (N) Change in dimension in direction i (mm)t Error in the specimen thickness (m)w Error in the width (m) =0 Error in the predicted strain at zero stress Error in the predicted intercept of stress-stain data (MPa)Error in the stress (MPa) Predicted intercept of stress-strain data (MPa) Engineering stress (MPa)Yield point (MPa) Ultimate strength (MPa)
2.0 IntroductionOne material property that is widely used and recognized is the strength of a material. But what does the word strength mean? Strength can have many meanings, so let us take a closer look at what is meant by the strength of a material. We will look at a very easy experiment that provides lots of information about the strength or the mechanical behavior of a material, called the tensile test.The basic idea of a tensile test is to place a sample of a material between two fixtures called grips which clamp the material.The material has known dimensions, like length and cross-sectional area.We then begin to apply weight to the material gripped at one end while the other end is fixed.We keep increasing the weight often called the load or force while at the same time measuring the change in length of the sample.The result of this test is a graph of load amount of weight versus displacement amount it stretched.Since the amount of weight needed to stretch the material depends on the size of the material and of course the properties of the material, comparison between materials can be very challenging.The ability to make a proper comparison can be very important to someone designing for structural applications where the material must withstand certain forces.
Figure 1: Standard tensile test specimen
3.0 Objectives
The purpose of this experiment is to :1.0 determine the tensile properties subjected to tensile loading.2.0 Identify Types of fracture surface under tensile loading.3.0 Validate the data between experimental and theoretical values.
4.0 TheoryCertain materials which are linear, homogeneous, elastic, and isotropic can bedescribed by their material properties. These properties include the modulus of elasticity, ultimate tensile strength, modulus of toughness, modulus of resilience and yield strength. Assuming mild steel is homogenous material, tensile testing had been carried out. One of important fundamental material Science is tensile testing which is carried out by applying uniaxial stress on the subject until it fracture such below. Figure 2: Sample mild steel shape
When force are applied to materials, it deform in reaction to those forces. This uniaxial stress also known as tensile stress is given by a formula of:(1)
While normal strain is given by:(2)
In theory, properties of material include the modulus of elasticity, modulus of toughness, modulus of resilience, ultimate tensile strength, and yield strength applied to all instances of that material undergoing the same type of stress, allowing one to design structural elements whose behaviour can be predicted but in at early stage of tested material will elongate to show elastic behaviour as the apply stress is proportional to the strain and Hookes law is obeyed. Hence this formula came:(3)
Figure 3: Stress-strain graph of mild steel
Elastic modulus, E also can be determine from Stress-strain graph which act as the gradient from the initial to limit of proportionality. As stress increasing, elastic behaviour stop at their elastic limit and entering plastic deformation. (4)E = slope =
Since many metals lack a sharp yields points, i.e a sudden, observable transition between the elastic region and the plastic region, the yields points is often defined as the stress that gives rise to a 0.2% permanent plastic strain. By this convention, a line is drawn parallel to the elastic region of the materials, starting at a strain level of 0.2% strain. The point at which this line intersects the curve is called the yield point or yield stress. The ultimate tensile strength( stress), in contrast is found by determining the maximum stress, reached by the materials.The ductility of the material can be measured most accurately from the tensile test using this definition:Ductility = Change in x-sectional area Original x-sectional area
This measure of ductility is closely related to one based upon the change in gage length divided by the original gage length, but after fracture the gage length is difficult to measure Tensile testing is very important because the performance of materials are a matter of life or death. Cars and airplanes cannot fail, and buildings must stay standing or it will cost life.
5.0 Experimental Procedure5.1 Apparatus/Experimental Setup
A G.U.N.T Hamburg Tensile Testing Machine (Max. load = 2kN), Vernier Caliper and specimen.
Figure 4: G.U.N.T Hamburg Tensile Testing Machine (Max. load = 2kN)
Figure 5: Specimen (aluminum)Figure 6: Vernier calliper
5.2 Procedure1. Vernier caliper used to measure the initial gage length, width and thickness of the test specimen.2. The specimen was mounted to the gripping grip of the machine.3. The load anchor was turned slowly to counter clockwise rotation until the specimen fixed in gripping head.(Notes: The specimen must lays correctly to the ground of the gripping head groove)4. Both gauges were reset to zero (extension gauge and load gauge).5. The wheel rotated until the extension gauge reading reached 10 units.6. Take and record the load reading7. Step 5 and 6 repeated until the specimen fracture.
Note that: Counter clockwise turning for tension, clockwise turning for compressive. Ratio for load gage: 1cm = 0.05N, dial gage: 1cm = 0.01
6.0 Data
w
tLo
Lo = 30mm, L = 42.9 mm, w = 3.14 mm, t = 1.06 mm, A = 3.33 mmNo.Extension(mm)Load (Kn)StrainStress (kPa)
10.10.10.003330030.03003
20.20.250.006775075.07508
30.30.40.0100120120.1201
40.40.50.0133150150.1502
50.50.550.0167165165.1652
60.60.550.0200165165.1652
70.70.550.0233165165.1652
80.80.60.0267180180.1802
90.90.60.0300180180.1802
1010.650.0333195195.1952
111.10.650.0367195195.1952
121.20.70.0400210210.2102
131.30.70.0433210210.2102
141.40.70.0467210210.2102
151.50.70.0500210210.2102
161.60.750.0533225225.2252
171.70.750.0567225225.2252
181.80.750.0600225225.2252
191.90.750.0633225225.2252
2020.750.0667225225.2252
212.10.80.0700240240.2402
222.20.80.0733240240.2402
232.30.80.0767240240.2402
242.40.80.0800240240.2402
252.50.80.0833240240.2402
262.60.80.0867240240.2402
272.70.80.0900240240.2402
282.80.850.0933255255.2553
292.90.850.0967255255.2553
3030.850.1000255255.2553
313.10.850.1033255255.2553
323.20.850.1067255255.2553
333.30.850.1100255255.2553
343.40.850.1133255255.2553
353.50.850.1167255255.2553
363.60.850.1200255255.2553
373.70.850.1233255255.2553
383.80.850.1267255255.2553
393.90.850.1300255255.2553
4040.850.1333255255.2553
414.10.850.1367255255.2553
424.20.850.1400255255.2553
434.30.90.1433270270.2703
444.40.90.1467270270.2703
454.50.90.1500270270.2703
464.60.90.1533270270.2703
474.70.90.1567270270.2703
484.80.90.1600270270.2703
494.90.90.1633270270.2703
5050.90.1667270270.2703
515.10.90.1700270270.2703
525.20.90.1733270270.2703
535.30.90.1767270270.2703
545.40.90.1800270270.2703
555.50.90.1833270270.2703
565.60.90.1867270270.2703
575.70.90.1900270270.2703
585.80.90.1933270270.2703
595.90.90.1967270270.2703
6060.90.2000270270.2703
616.10.90.2033270270.2703
626.20.90.2067270270.2703
636.30.90.2100270270.2703
646.40.90.2133270270.2703
656.50.90.2167270270.2703
666.60.90.2200270270.2703
676.70.90.2233270270.2703
686.80.90.2267270270.2703
696.90.90.2300270270.2703
7070.90.2333270270.2703
717.10.90.2367270270.2703
727.20.90.2400270270.2703
737.30.90.2433270270.2703
747.40.90.2467270270.2703
757.50.90.2500270270.2703
767.60.90.2533270270.2703
777.70.90.2567270270.2703
787.80.90.2600270270.2703
797.90.90.2633270270.2703
8080.90.2667270270.2703
818.10.90.2700270270.2703
828.20.90.2733270270.2703
838.30.90.2767270270.2703
848.40.90.2800270270.2703
858.50.90.2833270270.2703
868.60.90.2867270270.2703
878.70.950.2900285285.2853
888.80.950.2933285285.2853
898.90.950.2967285285.2853
9090.950.3000285285.2853
919.10.950.3033285285.2853
929.20.950.3067285285.2853
939.30.950.3100285285.2853
949.40.950.3133285285.2853
959.50.950.3167285285.2853
969.60.950.3200285285.2853
979.70.950.3233285285.2853
989.80.950.3267285285.2853
999.90.950.3300285285.2853
100100.950.3333285285.2853
10110.10.950.3367285285.2853
10210.20.950.3400285285.2853
10310.30.950.3433285285.2853
10410.40.950.3467285285.2853
10510.50.950.3500285285.2853
10610.60.950.3533285285.2853
10710.70.950.3567285285.2853
10810.80.950.3600285285.2853
10910.90.950.3633285285.2853
110110.950.3667285285.2853
11111.10.950.3700285285.2853
11211.20.950.3733285285.2853
11311.30.950.3767285285.2853
11411.40.950.3800285285.2853
11511.50.950.3833285285.2853
11611.60.950.3867285285.2853
11711.70.950.3900285285.2853
11811.80.950.3933285285.2853
11911.90.950.3967285285.2853
120120.950.4000285285.2853
12112.10.950.4033285285.2853
12212.20.950.4067285285.2853
12312.30.90.4100270270.2703
12412.40.90.4133270270.2703
12512.50.850.4167255255.2553
12612.60.850.4200255255.2553
12712.70.750.4233225225.2252
12812.80.70.4267210210.2102
12912.900.43000
Table 1: Data
Figure 7: Load(kN) vs Extension(mm) graph
Figure 8: Stress vs strain graph
The actual characteristic of the materials sample:The specimen used for this experiment is mild steel. The actual characteristic of the Mild steel is the most common form of steel as its price is relatively low while it provides material properties that are acceptable for many applications. Low carbon steel contains approximately 0.050.15% carbon and mild steel contains 0.160.29% carbon, therefore it is neither brittle nor ductile. Mild steel has a relatively low tensile strength, but it is cheap and malleable surface hardness can be increased through carburizing. It is often used when large amounts of steel is needed, for example as structural steel. The density of mild steel is 7,861.093kg/m (0.284lb/in), the tensile strength is a maximum of 500MPa (73,000psi) and the Young's modulus is 210,000MPa (30,000,000psi). Calculation of stress and strain:Area = (width x thickness) = 3.14 x 1.06 = 3.33 x 10-6 m2
7.0 References
1. Ashby, M. (2006). Engineering Materials 1: An Introduction to Properties, Applications and Design. 3rd ed. Butterworth-Heinemann2. Hibbeler, R.C. (2004). Statics and Mechanics of Materials. Prentice Hall.3. Tarr, M. (no date). Stress and its effect on Materials [online]. Available from4. http://www.ami.ac.uk/courses/topics/0124_seom/index.html. [Accessed 29/03/14].5. Van Vlack, L.H., Introduction to Materials Science and Engineering - 6th Edition, Addison Wesley, 1989, p 8.6. Smith,W.F., Principles of Materials Science and Engineering - 2nd Edition, McGraw Hill, 1990, p 255.7. Van Vlack, L.H., Introduction to Materials Science and Engineering - 6th Edition, Addison Wesley, 1989, p 556.8. Dewey, B. R., Introduction to Engineering Computing - 2nd Edition, McGraw-Hill, 1995, p 69.
8.0 AppendicesPage | 4