PPT: Stress & Strain

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 Page 1


TOPICS
• Topic cover
– Stress and strain
• Introduction to stress and strain, stress strain diagram
• Elasticity and plasticity and Hooke’s law
• Shear Stress and Shear strain
• Load and stress limit
• Axial force and deflection of body
– Torsion
• Introduction, round bar torsion, non-uniform torsion.
• Relation between Young’s Modulus E, ? and G
• Power transmission on round bar
Page 2


TOPICS
• Topic cover
– Stress and strain
• Introduction to stress and strain, stress strain diagram
• Elasticity and plasticity and Hooke’s law
• Shear Stress and Shear strain
• Load and stress limit
• Axial force and deflection of body
– Torsion
• Introduction, round bar torsion, non-uniform torsion.
• Relation between Young’s Modulus E, ? and G
• Power transmission on round bar
Stress and strain
DIRECT STRESS
? When a force is applied to an elastic body, the body deforms. The way in 
which the body deforms depends upon the type of force applied to it.
Compression force makes the body shorter.
A tensile force makes the body longer
?
Page 3


TOPICS
• Topic cover
– Stress and strain
• Introduction to stress and strain, stress strain diagram
• Elasticity and plasticity and Hooke’s law
• Shear Stress and Shear strain
• Load and stress limit
• Axial force and deflection of body
– Torsion
• Introduction, round bar torsion, non-uniform torsion.
• Relation between Young’s Modulus E, ? and G
• Power transmission on round bar
Stress and strain
DIRECT STRESS
? When a force is applied to an elastic body, the body deforms. The way in 
which the body deforms depends upon the type of force applied to it.
Compression force makes the body shorter.
A tensile force makes the body longer
?
A
F
Area
Force
Stress ? ? ? ?
2
/m N
Tensile and compressive forces are called DIRECT FORCES
Stress is the force per unit area upon which it acts.
….. Unit is Pascal (Pa) or 
Note: Most of engineering fields used kPa, MPa, GPa.
( Simbol – Sigma)
Page 4


TOPICS
• Topic cover
– Stress and strain
• Introduction to stress and strain, stress strain diagram
• Elasticity and plasticity and Hooke’s law
• Shear Stress and Shear strain
• Load and stress limit
• Axial force and deflection of body
– Torsion
• Introduction, round bar torsion, non-uniform torsion.
• Relation between Young’s Modulus E, ? and G
• Power transmission on round bar
Stress and strain
DIRECT STRESS
? When a force is applied to an elastic body, the body deforms. The way in 
which the body deforms depends upon the type of force applied to it.
Compression force makes the body shorter.
A tensile force makes the body longer
?
A
F
Area
Force
Stress ? ? ? ?
2
/m N
Tensile and compressive forces are called DIRECT FORCES
Stress is the force per unit area upon which it acts.
….. Unit is Pascal (Pa) or 
Note: Most of engineering fields used kPa, MPa, GPa.
( Simbol – Sigma)
?
L
x
Strain ? ? ?
?
DIRECT STRAIN , 
In each case, a force F produces a deformation x. In engineering, we 
usually change this force into stress and the deformation into strain 
and we define these as follows:
Strain is the deformation per unit of the original length.
The 
symbol
Strain has no unit’s since it is a ratio of length to length. Most 
engineering materials do not stretch very mush before they become 
damages, so strain values are very small figures. It is quite normal to 
change small numbers in to the exponent for 10
-6
( micro strain).
called EPSILON
Page 5


TOPICS
• Topic cover
– Stress and strain
• Introduction to stress and strain, stress strain diagram
• Elasticity and plasticity and Hooke’s law
• Shear Stress and Shear strain
• Load and stress limit
• Axial force and deflection of body
– Torsion
• Introduction, round bar torsion, non-uniform torsion.
• Relation between Young’s Modulus E, ? and G
• Power transmission on round bar
Stress and strain
DIRECT STRESS
? When a force is applied to an elastic body, the body deforms. The way in 
which the body deforms depends upon the type of force applied to it.
Compression force makes the body shorter.
A tensile force makes the body longer
?
A
F
Area
Force
Stress ? ? ? ?
2
/m N
Tensile and compressive forces are called DIRECT FORCES
Stress is the force per unit area upon which it acts.
….. Unit is Pascal (Pa) or 
Note: Most of engineering fields used kPa, MPa, GPa.
( Simbol – Sigma)
?
L
x
Strain ? ? ?
?
DIRECT STRAIN , 
In each case, a force F produces a deformation x. In engineering, we 
usually change this force into stress and the deformation into strain 
and we define these as follows:
Strain is the deformation per unit of the original length.
The 
symbol
Strain has no unit’s since it is a ratio of length to length. Most 
engineering materials do not stretch very mush before they become 
damages, so strain values are very small figures. It is quite normal to 
change small numbers in to the exponent for 10
-6
( micro strain).
called EPSILON
MODULUS OF ELASTICITY (E)
•Elastic materials always spring back into shape when released. 
They also obey HOOKE’s LAW. 
•This is the law of spring which states that deformation is directly 
proportional to the force. F/x = stiffness = kN/m
•The stiffness is different for the different material and different sizes of the 
material. We may eliminate the size by using stress and strain instead of 
force and deformation:
•If F and x is refer to the direct stress and strain , then 
A F ? ?
L x ? ?
L
A
x
F
?
?
?
?
?
?
Ax
FL
hence and 
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FAQs on PPT: Stress & Strain

1. What's the difference between stress and strain in strength of materials?
Ans. Stress is the internal force per unit area that acts on a material when external load is applied, while strain is the deformation or change in shape that results from that stress. Stress causes strain-think of stress as the "push" and strain as the material's "response" to that push.
2. How do I calculate tensile stress and what formula should I use?
Ans. Tensile stress equals the applied force divided by the original cross-sectional area: σ = F/A, where σ is stress in pascals, F is force in newtons, and A is area in square metres. This measures how much the material resists being pulled apart under tension.
3. Why does a material experience elastic deformation instead of permanent damage?
Ans. Elastic deformation occurs when stress remains below the elastic limit, allowing atomic bonds to stretch temporarily without breaking. Once the load is removed, these bonds return to their original positions, restoring the material's original shape and size completely.
4. What's the real difference between longitudinal strain and lateral strain when materials are stretched?
Ans. Longitudinal strain measures length change along the direction of applied force, calculated as ΔL/L₀. Lateral strain measures width or thickness reduction perpendicular to the force direction. When a rod is pulled lengthwise, it gets longer (longitudinal) but thinner (lateral) simultaneously.
5. How do Poisson's ratio and the stress-strain curve help predict material behaviour during exams?
Ans. Poisson's ratio (ν) quantifies the relationship between lateral and longitudinal strain, revealing how materials deform in all directions. The stress-strain curve visually shows elastic region, yield point, and fracture point, helping students identify material properties and predict failure modes instantly.
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