Material Science: Stress, Strain, and Moduli, Slides of Physics

An overview of various material properties, including stress, strain, young's modulus, spring constant, shear modulus, and bulk modulus. It discusses the relationship between stress and strain, the concept of elastic and inelastic materials, and the application of these concepts to real-world examples like bones and steel.

Typology: Slides

2012/2013

Uploaded on 07/12/2013

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Material Strength
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Material Strength

Stress vs Strain

^

A graph of stress versusstrain is linear for smallstresses. ^

The slope of stress versusstrain is a

modulus

that

depends on the type ofmaterial. ^

For normal stress this isYoung’s modulus

Y

^ 

Y

 Stress

Strain



stiff material

elasticmaterial

Inelastic Material

^

The linear behavior ofmaterials only lasts up to acertain strength – the

yield

strength

^

Materials can continue todeform but they won’t restoretheir shape. ^

For very high strain amaterial will break.

 Stress

Strain

breakingstrength 

yieldstrength

Shear Modulus

^

Materials also have amodulus from shear forces. ^

Shear modulus

S

also

matches with a springconstant. ^

The angle

^

=^

x

/ L

is

sometimes used for shear.

F^

x A^ (goes into screen) L

x

k

x

SA L

F

x

FLA

L

x

A

F

S

s s

 ^ 

Bulk Modulus

^

Pressure changes volume,not length. ^

Bulk modulus

B

relates

changes in pressure andvolume. ^

The negative sign representsthe decrease in volume withincreasing pressure.

P

V V A^ (surface area)

V

P V

V

V

A

F

B

V V

 

Under Pressure ^

Steel has a bulk modulus of B^

= 60 GPa. A sphere with a volume of 0.50 m

3 is

constructed and lowered intothe ocean where

P

MPa. ^

How much does the volumechange?

^

Use the relation for bulkmodulus.^ 

B

= -(

P

) / (

V

/ V

)

^

V

= -

V^

P

/^ B

^

Substitute values:^ 

(-0.50 m

3 )(2.0 x 10

7 Pa) /

(6.0 x 10

10

Pa)

^

V

= -1.6 x 10

4 m

3