mechanical properties of materials

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35 Terms

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stress

σ=FA0\sigma=\frac{F}{A_0}


F: force (N)

σ\sigma: stress (PaPa)

A0A_0: Area in square meters (m2m²)

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strain

Ɛ=l1−l0l0=Δll0\char"0190 =\frac{l_1-l_0}{l_0}=\frac{\Delta l}{l_0}


Ɛ\char"0190: strain (unitless)

ll, l0l_0, Δl\Delta l : length (mm)


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shear stress

τ=FA0\tau=\frac{F}{A_0}


τ\tau: shear stress (PaPa)

σ\sigma: stress (PaPa)

A0A_0: square meters (m2m²)

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shear strain

γ=tan⁡θ\gamma=\tan\theta


γ\gamma: shear strain (dimensionless)

θ\theta: angle (in degreesdegrees or radians: radrad)

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1MPaMPa=

1MPa=106Pa=106N1MPa=10^6Pa=10^6N /m2m²

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tension

pulling force that causes elongation

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compression

pushing force that causes shortening

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torsion

twisting around the longitudinal axis

Example : holding one end of a metal stationary while twisting the other end


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load cell

measures applied force FF in newtons (N)

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extensometer

measures elongation Δl\Delta l in mmmm or mm

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imagine you have a steel rod holding up a very heavy object.

why do mechanical properties matter?

when force is applied, the rod might:

  • stretch (elongate)

  • shorten (compress)

  • change shape (deform)

  • break (fracture)

engineers need to understand how materials respond to forces so they can prevent excessive deformation and fracture.


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what affects a material's mechanical behavior?

  • nature of load: (type of force) whether the material is pulled, pushes, or sheared, and whether the force changes


  • duration: how long the load is applied (from seconds to years)


  • environment: temperature and surrounding conditions


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a) what is ATSM

b) why does it matter

a) ATSM: American society for testing and materials.

it develops and publishes standards for testing materials.


b) to compare results fairly, we need consistent testing procedures.

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what do structural engineers do?

  1. determine stresses and stress distributions in loaded structures.

  2. use experimental testing and mathematical analysis.

  3. select materials with suitable combinations of mechanical properties


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4 types of loading

knowt flashcard image
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tension tests

a tension test measures how a material behaves when it is pulled until it deforms or fractures


the middle section is narrower than it ends so that we can concentrate the deformation in the middle rather than near the grips


the machine gradually increases its tensile load, while measurements are recorded.

<p>a tension test measures how a material behaves when it is pulled until it deforms or fractures</p><p></p><p>the middle section is narrower than it ends so that we can concentrate the deformation in the middle rather than near the grips</p><p></p><p>the machine gradually increases its tensile load, while measurements are recorded.</p>
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parts of the testing machine

instruments:

  • load cell: measures the applied force FF

  • extensometer: measures elongation Δl\Delta l


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characteristics of a tensile test

  • the specimen elongates at a constant rate

  • the test typically lasts several minutes.

  • it is


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Area of a circle

A=πR2A=\pi R^2

R=d2R=\frac{d}{2}

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Comparison test

A comparison test measures how a material behaves when a pushing force is applied

<p>A comparison test measures how a material behaves when a pushing force is applied</p>
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-ve stress or strain

-ve answers ←→ Compression

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When are compressive tests used?

  • compressive service loads: when the material will experience pushing forces in real/actual uses

  • Large plastic deformation: when studying permanent (plastic) deformation, such as metal forming

  • Brittle materials: when tensile testing is impractical, such as with ceramics or cast iron


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Which test is more common? Why?

Tensile tests are more common


  • they are easier to perform and instrument

  • For most structural metals, compression tests provide little additional information


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What is shear?

Shear occurs when forces are applied parallel to a material’s surface → causing angular distortion

<p>Shear occurs when forces are applied parallel to a material’s surface → causing angular distortion </p>
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Normal stress vs shear stress

They have identical formulas but…

Normal stress → force acts perpendicular to the cross section

Shear stress → force acts parallel to the surface

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Elastic deformation

Temporary deformation (reversible)


When applied force is removed → material returns to it’s original shape and dimensions


Ex: stretching a spring and (applied force) then releasing it (removing applied force → back to its original form)

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Hook’s law

σ=Eε\sigma=E\varepsilon


σ\sigma: normal stress (MPa)

E: Young’s modulus (modulus of elasticity) (MPa)

ε\varepsilon: normal strain (unitless)





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Young’s modulus

Modulus of elasticity EE: measures stiffness

Higher EE → stiffer material → less strain for the same stress

Lower EE → less stiff material → more strain for the same stress

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Stress - strain graph

SLOPE=ΔσΔε=ESLOPE=\frac{\Delta\sigma}{\Delta\varepsilon}=E


So if the question gives a straight line stress-strain graph and asks for stiffness (EE) calculate its slope.

<p>$$SLOPE=\frac{\Delta\sigma}{\Delta\varepsilon}=E$$ </p><p></p><p>So if the question gives a straight line stress-strain graph and asks for stiffness ($$E$$) calculate its slope.</p>
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Non Linear elastic behavior

Some materials (cast iron, concrete, polymers) exhibit nonlinear elastic behavior


For a point (ε\varepsilon,σ\sigma) → secant modulus → Esec⁡ant=σεE_{\sec ant}=\frac{\sigma}{\varepsilon}


For a point (ε\varepsilon,σ\sigma) → tangent modulus is the slope at that point→ Etan⁡gent=dσdεE_{\tan gent}=\frac{d\sigma}{d\varepsilon}


<p>Some materials (cast iron, concrete, polymers) exhibit nonlinear elastic behavior</p><p></p><p>For a point ($$\varepsilon$$,$$\sigma$$) → secant modulus → $$E_{\sec ant}=\frac{\sigma}{\varepsilon}$$</p><p></p><p>For a point ($$\varepsilon$$,$$\sigma$$) → tangent modulus is the slope at that point→ $$E_{\tan gent}=\frac{d\sigma}{d\varepsilon}$$</p><p></p>
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Why are some materials stiffer than others?

Because it depends on interatomic bonding forces.


E∝(dFdr)r0E\varpropto\left(\frac{dF}{dr}\right)_{r_0}


F: interatomic force (N)

rr: atomic separation (m)

r0r_0: equilibrium separation (m)


Stronger bonds → higher modulus EE

Weaker bonds → lower modulus EE

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Temperature and shear modulus

As temp increases:

  • atomic vibrations increase

  • Effective bond stiffness decreases

  • Modulus EE decreases

TT increases → EE decreases


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Shear modulus

τ=Gγ\tau=G\gamma → G=τγG=\frac{\tau}{\gamma}

GG: shear modulus (MPa)

τ\tau: shear stress (MPa)

γ\gamma: shear strain (unitless)




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Anelasticity

Anelasticity: delayed elastic response and delayed recovery (unlike elastic deformation which recovers immediately)

  • strain can continue increasing after a load is applied

  • Recovery takes time after the load is removed

  • The material eventually goes back to its original form


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