exl graph (engineering) in a lab report

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example_of_old_report_.docx

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:

C:\Users\jma86517\Desktop\steel.PNG

Figure 1: Stress-strain curve for 1018 Steel

C:\Users\jma86517\Desktop\alum.PNG

Figure 2: Stress-strain curve for 2024 Aluminum

C:\Users\jma86517\Desktop\LPDE.PNG

Figure 3: Stress-strain curve for LDPE

C:\Users\jma86517\Desktop\HDPE.PNG

Figure 4: Stress-strain curve for HDPE