exl graph (engineering) in a lab report
Alrashaid 1
Alrashaid 2
Alrashaid 3
Theories:
Engineering Stress : σ = P/A0,
True Stress : σ T = P/AT, σ T = σ (1+ ϵ ).
True Stress: ϵ = (lf – l0) / l0.
True train: ϵ t = ln (li/l0) = ln (1+ ϵ).
Precent elongation= ((lf – l0) / l0) *
Precent Error = ((|Experimental Value – Theoretical Value|)/Theoretical Value)*
Modulus of elasticity E = slope of young’s modulus line in stress vs strain curve
Discussion:
By observing the stress-strain curves the different tensil properties for the various tested materials can be seen. The material with the largest ultimate tensile strength is steel shown in Figure 1. What can be noticed on the curve of this particular specimen is the the wavey distortions before the curve reaches the ultimate tensile stress. This is due to the properties of steel in which some discontinuities within the grain structure and impurities within the sample are formed which yielded almost constant strain under the increasing tensile load. This happens with the aluminun sample but in a lesser manner. Steel also experiences more necking before failure comparinng it with the Aluminum sample. It can be cunclueded that Aluminum was more brittle than steel. Both polymers LDPE and HDPE have a largees plastic region, which means they deforem a lot more before faluir accures in comparison with thhe steel and aluminum sample. This can be seen in figures 3 and 4 The table below shows all the calculations done that helped in forming the graphs.
|
Specimen |
Width (in) |
Thickness (in) |
Area (in^2) |
Lo |
Lf |
%Elongation |
|
Steel 1018 |
0.503 |
0.125 |
0.062875 |
3.79 |
4.7050955 |
24.145 |
|
LDPE |
0.839 |
0.129 |
0.108231 |
3.75 |
10.2133125 |
172.355 |
|
Al 2024 |
0.505 |
0.127 |
0.064135 |
3.75 |
4.5742125 |
21.979 |
|
HDPE |
0.737 |
0.12 |
0.08844 |
3.75 |
10.3402875 |
175.741 |
|
Fail load (lb) |
ENG stress (psi) |
Strain (psi) |
ENG strain (psi) |
True strain |
True stress |
|
3985.367 |
63385.55865 |
17.14908 |
0.1714908 |
0.158277126 |
74255.59881 |
|
152.1301 |
1405.605603 |
19.40467 |
0.1940467 |
0.177348126 |
1678.358732 |
|
4111.328 |
64104.28003 |
20.44067 |
0.2044067 |
0.185987081 |
77207.62437 |
|
343.628 |
3885.436454 |
12.256 |
0.12256 |
0.115611791 |
4361.635546 |
Young’s modulus for the matrials was alos calculated. This was done by taking the slope of young’s modulus line in stress vs strain curve shown in figures 1, 2, 3, and 4. The calculated values were campared to the given values and the error was obtained. The below table shows the results :
|
Material |
Calculated Modulus |
Given Modulus |
Error % |
|
1018 steel |
1940785.802 |
29000000 |
93.30764 |
|
2024 Aluminum |
212019.4049 |
1000000 |
78.79806 |
|
LDPE |
30897.88491 |
80000 |
61.37764 |
|
HDPE |
159807.4659 |
145000 |
10.21205 |
Figures:
Figure 1: Stress-strain curve for 1018 Steel
Figure 2: Stress-strain curve for 2024 Aluminum
Figure 3: Stress-strain curve for LDPE
Figure 4: Stress-strain curve for HDPE