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Experiment no 1:

object:
To study Olsen Universal Testing Machine and it’s operation.

Apparatus:
Tinius Olsen Universal Testing Machine

Theory:
This universal testing machine is intended only for static type of mechanical tests. The loading is done by hydraulic mechanism. This machine can be adopted for many special applications and a large variety of tests can be performed on this machine using proper attachments, for example tensile test, bending test, shearing test, torsion test.

Components:

Loading Mechanism:

The loading application is accomplished by a hydraulic piston & cylinder located at the base. The hydraulic pressure is developed by a gear pump. The pump in combination with automatic valve provided uniform rates of loading. Safety valves protect the gauges from overload. The speed of loading is controlled by pilot hand wheel and due to this valve arrangement (load/unload), load may be easily applied and removed or held constant. Construction of entire loading unit is very rugged and compact. Hydraulic oil of Grade SAE 40 is used. The capacity of oil reservoir is 13 gallons.

Indicating Mechanism:

Loads on Universal testing machine are indicated on precision type hydraulic gauges, which are mounted on the instrument panel. These gauges are provided with maximum pointers.

Operation:

Loads on this machine are indicated on two hydraulic gauges. Application of all test loads (compression/tension) is accompanied by the upward movement of piston. The lower cross heads may be adjusted by using cross head adjusting crank to any desired position. For tensile loading the test specimen is mounted on the upper side on the lower head. For compressive loading the test specimen is mounted on the lower side of lower head.

Zero Setting:

All zero setting must be made with specimen, testing.

Shut Down:

Close the load completely. Open the unload valve slowly and gradually. After piston completely sets to its seat (the load pointer suddenly drops below the zero load mark). Close the unload valve. Stop the pump by pressing the stop button. Close the gauge valve.

Care and Maintenance: Object:
To determine the Modulus of Elasticity of a given specimen and draw stress-strain diagram.

Apparatus:
Universal Testing Machine, given specimen

Theory:
In the course of operation all articles are subject to the action of external forces, which creates stresses that inevitably cause deformation. To keep these stresses within permissible limits, it is necessary to select suitable material. A comprehensive knowledge of mechanical characteristics of metal products (strength, ductility, malleability, creep etc.) is essential for this purpose. The mechanical properties quoted in different books of materials are based on different mechanical tests.

Mechanical tests are those in which specially prepared specimens of standard size are tested on special machine to obtain different mechanical properties of metals. Mechanical tests are conducted under various loading conditions. They may be:

Tensile Test: Considerable information about the properties of a material can be obtained from uniaxial tensile test. Tensile test is of static type, i.e., load is increased slowly from zero to a certain final value. Standard specimens are designed to produce uniform uniaxial tension in the central portion and to ensure reduced stresses in the sections is gripped. The mechanical properties in tension are determined on the gauge loading.

After loading is applied, it will be noted that up to a certain stress, the strain is directly proportional to stress (obeys Hooke’s law).

After plotting strain on horizontal axis and stress on vertical axis, the prominent features of a stress-strain curve are:

Observation: For Aluminum
Load 
Extension
Load
Extension
(lbs)
(in)
(lbs)
(in)
0
0
2100
213
100
32
2200
229
200
38
2300
247
300
46
2400
265
400
53
2500
280
500
62
2600
298
600
70
2700
320
700
78
2800
344
800
86
2900
371
900
94
3000
394
1000
103
3100
428
1100
111
3200
471
1200
120
3300
538
1300
128
3380
680
1400
137
3300
706
1500
146
3200
730
1600
156
3100
745
1700
164
3000
760
1800
173
2900
772
1900
187
2800
782
2000
200
2700
796
Calculations:
Stress = Force/Area
Strain = Change in length/Original Length For Aluminum:
Stress
Strain
Stress
Strain
lb/in2
lb/in2
0
0
19004.52
0.1065
904.978
0.016
19909.5
0.1145
1809.95
0.019
20814.48
0.1235
2714.93
0.023
21719.45
0.1325
3619.9
0.0265
22624.43
0.14
4527.89
0.031
23529.41
0.149
5429.87
0.035
24434.39
0.16
6334.84
0.039
25339.37
0.172
7239.82
0.043
26244.34
0.1855
8144.79
0.047
27149.32
0.197
9049.77
0.0515
28054.29
0.214
9954.75
0.0555
28959.27
0.2355
10859.73
0.06
29864.25
0.269
11764.7
0.064
30588.24
0.34
12669.69
0.0685
29864.25
0.353
13574.66
0.073
28959.27
0.265
14479.6
0.078
28054.29
0.3725
15384.61
0.082
27149.32
0.38
16289.59
0.0865
26244.34
0.386
17194.57
0.0935
25339.37
0.391
18099.54
0.1
24434.39
0.398

        E =     Stress
                  Strain

Graphically

E = 4000/0.03

= 133.333 kips

For Mild Steel

Stress
Strain
Stress
Strain
Lb/in2
lb/in2
0
0
59675
0.1125
3978
0.009
63653
0.1195
7956
0.018
67632
0.125
11935
0.028
71610
0.132
15913
0.038
75588
0.1385
19891
0.045
79567
0.1455
23870
0.0525
83545
0.151
27848
0.0595
87523
0.1595
31826
0.0655
91502
0.165
35805
0.073
95480
0.1735
39783
0.08
91502
0.2235
43761
0.0865
87523
0.2395
47740
0.0935
83545
0.2475
51718
0.1
79567
0.2575
55697
0.106
75588
0.265
71610
0.2725
E = Stress
      Strain
Graphically

E = 39783/0.08

= 497.287 kips
 
 


EXPERIMENT NO. 3



OBJECT:

To determine the shear stress of given wooden specimen.

APPARATUS:

Universal testing machine, wooden shearing attachment, wooden specimen.

THEORY:

Shear stress: The stress that is caused by forces acting along or parallel to the area.

Or

Internal reacting shear force is expressed as force per unit area.

It is also termed as tangential stress.

A shearing stress is produced whenever applied loads cause one section of body to tend to slide past its adjacent section.

Properties of timber:

Timber has been used as a structural material since pre historic times. We use more wood than we do any other engineering material. Wood has three noticeable characteristics

Natural wood is a complex fiber reinforced material. Hard wood is obtained from deciduous trees & softwood obtained from evergreen, have similar structure.

Several factors influence the behavior of wood. The moisture content in timber, age of timber & type of timber. During drying, the wood shrinks & cracking may occur.

Wood is highly anisotropic. Because of the orientation of fibers, the strength in longitudinal (lengthwise) direction is may be about 25-50 times greater than the strength in the radial or tangential (sidewise) direction.

However clear wood composite of fiber & lignin & free from imperfection such as knots has longitudinal tensile strength of 10,000 psi to 20,000 psi. strength in tension is superior to either compression or shear. In compression fibers buckle, in shear the fibers sliding past one another.

SPECIMEN & ATTACHMENT:

A parallel to grain specimen is prepared to test as prescribed in ASTM methods. Attachment used in this test is very specialized & also used to determine shear strength of adhesives of bonding wood. The specimen is placed in the tool with lower under the flat blade. Minor misalignment is of wooden block is automatically compensated by semicircular blade which assures uniforms lateral distribution of load. In use tool is placed on the testing machine table & load is applied in compression against the blade. Provision is made to mount the blade on the lower crosshead.

Observation/calculation:

Shear load: 5480 lbs.

Shear area: 4 in².

Shear stress for given wooden specimen = shear load =1620 psi

shear area

Result:- Shear stress for the given specimen of wood is found to be 1620 psi
 
 




EXPERIMENT NO 4

OBJECT:

To determine the single shear strength of given 1/2" dia aluminum, mild steel and brass bar.

APPARATUS:

Universal testing machine, Bar shearing attachment, Allen key, Specimen.

WORKING FORMULA:

Single share stress

t =F/A (lb/in2)

Where

t = Share stress

F = Applied Force

A = Cross sectional area

BAR SHEARING PROCESS:

The shearing process starts when blade (upper cutting edge) descends against bar, the metal first deformed plastically over the die (lower cutting edge). Due to small lateral clearance between the two cutting edges, the deformation is highly localized. The blade (upper cutting edge) penetrates into the bar and opposite surface bulges slightly. When penetration reaches 15% to 60% of diameter of bar (depending upon properties of material), the applied force exceeds the shear resistive force of the metal and metal suddenly shears or ruptures through remainder of its diameter. Due to non-homogeneity in the metal, the final phase of shearing doesn’t occur uniformly.

BAR SHEARING TOOL:

Bar shearing tool comprises of shearing blade (upper cutting edge) & bar holding base (contains lower cutting edge i.e. die also serve to hold bar firmly during course of practical). The shearing blade have precision notches in all four sides, are used for ¼", ½", 3/4" & 1" diameter bars for testing in single or double shear. Shearing blade &die are made of tempered tool steel. They are ground to true edge.

SPECIMEN & ATTACHMENT:

A parallel to grain specimen is prepared for test as prescribed in ASTM

Methods. Attachment used in this test is very specialized and also used to determine shear strength of adhesives of bonding wood. The specimen is placed in the tool with lower portion under the flat blade. Minor misalignment is of wooden block is automatically compensated by semicircular blade which assure uniform lateral distribution of load. In use tool is placed on the testing machine table and load is applied compression against the blade. Provision is made to mount the blade on the lower crosshead.

OBSERVATION:
 
Specimen
Loads(lbs)
Diameter(in)
Shear stress(psi)
Mild Steel
13700 lbs
0.5 in
26.73 ksi
Brass
10000 lbs
0.507 in
69.77 ksi
Aluminium
5240 lbs
0.5 in
49.38 ksi

RESULT:

  1. Shear stress of aluminum = t a = 26.73 ksi
  2. Shear stress of mild steel = t s = 69.77 ksi
  3. Shear stress of brass = t b = 49.38 ksi

 

EXPERIMENT NO: 5a

OBJECT:

To determine hardness of different materials.

APPARATUS:

Hardness testing machine, Specimen, Indenter with different diameter balls.

THEORY:

Hardness is the resistance to penetration. Hardness tests give measure of the resistance of a metal to the penetration & resistance to scratching or abrasion.

The Brinell hardness test is of static indentation type. It is one of the most widely used hardness tests in engineering practice.

The Brinell hardness test is basically simple and consists of applying constant load, usually 500 to 3000 kg on a hardened steel ball type indenter, 10 mm in diameter, to the flat surface of a work piece. The 500-kg load is used for testing non-ferrous metals such as copper, aluminum alloys, whereas 3000-kg load is for testing harder metals such as steel, cast iron etc.. The load is held for a specified period of time (10 to 15 sec. for iron or steel, about 30 sec. for softer metals) after which the diameter of recovered indentation is measured in mm. This time period is required to ensure that plastic flow of the work metal has stopped.

Hardness is evaluated by taking the mean diameter of the indentation (two readings at right angles to each other) & calculating Brinell hardness number (HB) by dividing applied load by the surface area of indentation, as per formula:

HB = load .

( p D / 2 ) [ D - ( D2 – d2 ) ]

Where D = Diameter of the ball in mm.

d = Diameter of the indentation in mm.

For the selection for Brinell hardness test, following chart is very helpful:
 
REPRESENTATIVE MATERIAL
P / D2
BALL DIAMETER
LOAD (Kgf)
Steel & cast iron
30
2.5 mm
187.5
Copper, copper & Aluminum alloy
10
5 mm
250
Aluminum
5
5 mm
125

Lead, tin & their alloy
1
10 mm
100

PROCEDURE:

  1. Check that the major load lever is down.
  2. Select the load required.
  3. Push the quick lift lever fully toward the machine body.
  4. Place the specimen to be rested on the anvil.
  5. Rotate the capstan wheel clockwise until the specimen is in contact with the intender.
  6. Lift the major load lever gently until it moves independently.
  7. Allow the major load to dwell & then push the major load down gently to its stop dwell line depend on type of material.
  8. Rotate the capstan wheel anticlockwise to lower the specimen from the anvil.
  9. Remove the specimen from the anvil. The diameter of the indentation left in the surface after the removal of load is measured in two directions at right angles.
  10. Substitute the values in the formula given. The quotient obtained is the Brinell hardness number.

  11. HB = load .

    ( p D / 2 ) [ D - ( D2 – d2 )½]

    Where D = Diameter of the ball in mm.

    d = Diameter of the indentation in mm.

  12. The Brinell hardness number can be written as:
(Quotient) HB (Diameter of ball used) / (Load applied)

OBSERVATION CHART:
 
Material
Mild Steel
Stainless Steel
Aluminum
Brass
Load (P) Kgf
187.5
187.5
125
250
Diameter of Ball (D) 

mm.

2.5
2.5
5
5
Diameter of Indentation (d) mm.
1.2
1.35
1.35
1.5
Brinell Hardness No. 
155.612
120.621
103.74
207.483

 

RESULT:

The Brinell hardness number of different materials is found to be
 
Mild Steel
Stainless Steel
Aluminum
Brass
155.612
120.621
103.74
207.483

 
 
 

EXPERIMENT NO 5(b)

OBJECT:

To determine Hardness of different materials by " Rockwell Method."

APPARATUS:

Hardness tester, Specimen, Different indenter.

THEORY:

Hardness is the resistance to penetration. Hardness tests give measures of the resistance of a metal to the penetration & resistance to scratching or abrasion.

The Rockwell hardness test is of static indentation type. It is one of the most widely used hardness tests in engineering practice.

Rockwell hardness differs from Brinell hardness testing in that hardness is determine by the

depth of indentation made by a constant load impressed upon indenter rather than surface area of indentation. Rockwell test consists of measuring the additional depth to which an indenter is forced by heavy (major) load beyond the depth of previously light (minor) load. Application of minor load eliminates backlash in the load train and causes indenter to breakthrough slight surface roughness and to crush particles of foreign matter. Thus contributing greater accuracy in the test.

In regular Rockwell hardness test the minor load is always 10 kg. The major load however can be 60,000 or 150 kg. Depending upon the type of scale used (selection of scale is done according to type of material).

SELECTION OF ROCKWELL SCALE:

It is necessary to select the Rockwell scale to suit a given set of circumstances. Therefore knowledge of the factors that govern the proper choice of scale is mandatory. There are 15 different scale of regular Rockwell hardness is available. The influencing factors which governs the selection of Rockwell scale is:

Among 15 different scales for regular Rockwell testing here are some with typical applications:
Scale
Indenter
Major Load
Application
B
Ball ( 1/16'' )
100 Kg
Cu alloy , soft steel,Al alloy ,malleable iron
C
Diamond cone
150 Kg
Steels , Hard cast iron,titanium,hardened steel
A
Diamond cone
60 Kg
Cemented Carbide ,Thin steels
D
Diamond cone
100 Kg
Pearlitic malleable iron
E
Ball ( 1/8 '' )
100 Kg
Cast iron ,Al & Mg alloys , bearing metals

For ball indenter red dial graduation. For diamond cone indenter black dial graduations.

PROCEDURE:

  1. Check that the major load lever is down.
  2. Select the load required (as per type of material).
  3. Push the quick lifts level fully downs the machine body.
  4. Place specimen to be tested on the anvil.
  5. Rotate the capstan wheel clockwise until the specimen is in contact with the indenter. Continue to rotate the capstan wheel gently until the small hand (automatic zero hand) is about half way among the red zone.
  6. Turn the dial face so the "0" on the dial lines up with the large dial hand.
  7. Lift the major load lever gently until it moves independently.
  8. Allow the major load to dwell and then push the major load down gently to its stop. Dwell time depends on type of material.
  9. Rockwell hardness number can be read directly from the dial. Note down the reading.
  10. Rotate the capstan wheel anti clock wise to lower the specimen from the
indenter.

The Rockwell hardness number can be represented as:

OBSERVATION:
 
Material 
Load
Indenter
Angle
Rockwell Hardness
(HRC)
High Carbon Steel
150
Diamond
120
43
Spring steel
150
Diamond
120
26

 

RESULT:

The Rockwell hardness number of different material are found to be:

For High Carbon Steel = 43

For Spring Steel = 26

EXPERIMENT NO: 6

Object:

To determine modulus of rigidity of given material by method torsion.

Apparatus:

Torsion apparatus, load.

Theory:

Torsion is the shear produced by rotation or by a torque. In this type of shear,one layer of a material is made to rotate on an adjection layer. This type of shear is present in rotating shafts when transmitting power.

In torsion test, equal and opposing moments are applied at opposing ends of a suitable specimen in planes perpendicular to its longitudinal axis. Observation of applied torque and corresponding twist or rotation is used to determine modulus of rupture, modulus of rigidity and angle of twist of given material.

Torsion formula:

Torsion formula is used for determining Modulus of Rigidity of given material.

T/J = Gq /L = t /r

Where:

T = Torsion lb.-in

J = Polar moment of inertia in4

t = Shear stress . Psi.

G = Modulus of rigidity. Psi.

q = Angle of twist. Rad.

L = Length of shaft in..

r = Radius of shaft in..

The assumptions that are made for the formulation of torsion formula are as under :

Modulus of Rigidity:

Modulus of Rigidity is define as:

The relationship between shearing stress & shearing strain, assuming

HOOKE’S LAW to apply to shear is :

t = G g

where:

G represents modulus of elasticity in shear OR Modulus of rigidity.


OBSERVATION:
 
Weight
L1 
L2 
q 1
q 2
Torque 
G1 
G2 
(lbs)
(in) 
(in)
(rad)
(rad)
(lb-in)
(psi)
(psi)
8.8
10
20
0.008
0.026
31.35
1.15
0.78
17.6
10
20
0.026
0.061
62.7
0.78
0.66
26.4
10
20
0.043
0.096
94.05
0.69
0.63

Calculations:

Polar moment of inertia = p /2 r 4 = p /2 (3/8)4 =.0321 in4

G 1 = 874.33 ksi

G 2 =691 ksi

Mean G = ( G 1+ G 2) /2 = 782.66

Result:

Modulus of elasticity in shear OR Modulus of rigidity of given material

Is found to be = 782.66 ksi