i.pengujiansifatmekanik
TRANSCRIPT
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Pengujian Materials
• Definition - normal load, shear load
- tension, compression
- stress, strain
• Stress and Strain Diagram• Material Characteristics
- ductility
- brittleness
- toughness - transition temperature
- endurance limit
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• Normal Load (Axial load) : Load is perpendicular to the
supporting material
! Tension Load : As the ends of material are pulled apart
to ma"e the material longer# the load is called a tension
load
! Compression Load : As the ends of material are pushed in to ma"e the material smaller# the load is called
a compression load
Tension
Compression
5.1 Classifying Load
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• Shear Load : $angential load
5.1 Classifying Load (cont)
pulling apart
Pressure
Cargo
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5.2 Stress and Strain
%n order to compare materials# &e must ha'e measures
• Stress : load per unit Area
A
Fσ =
F : load applied in pounds
A : cross sectional area in in²
: stress in psiσ
A
F F
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5.2 Stress and Strain (cont)
• Strain :! Ratio of elongation of a material to the original length
- unit deformation
oL
e
ε =
e : elongation (ft
Lo : unloaded(original length of a material (ft
: strain (ft!ft or (in!in
ε Elongation
oLLe −=
L : loaded length of a material (ft
Lo e
L
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"ald#in $ydraulic %achine for &ension ' Compression test
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5.3 Stress-Strain Diagram
• A plot of Strain 's Stress
•$he diagram gi'es us the eha'ior of the material and
material properties
• ach material produces a different stress!strain
diagram
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5.3 Stress-Strain Diagram
Strain ( ) (eLo)
)
*
+
S t r e s s
( F A )
lastic
*egion
Plastic
*egion
Strain
+ardening ,racture
ultimatetensilestrength
S l o
p e -
!
lastic region
slope./oung0s(elastic modulus
yield strength
Plastic region ultimate tensile strength
strain hardening
fracture
nec1ing
yieldstrength
2&3σ
yσ
ε!σ =
ε
σ! =
ε 12
y
ε ε
σ
!−
=
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A+4 3teel
3tress and 3train 5iagram
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5.3 Stress-Strain Diagram (cont)
• !lasti" #egion (Point . /0)
! $he material &ill return to its original shape
after the material is unloaded( li"e a ruer and)
! $he stress is linearl1 proportional to the strain in
this region
ε!σ =
: Stress(psi)
! : Elastic modulus (Young’s Modulus) (psi)
: Strain (in2in)
σ
ε
- Point 0 : 3ield Strength : a point at &hich permanent
deformation occurs ( %f it is passed# the material &ill
no longer return to its original length)
ε
σ! =or
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• $lasti" #egion (Point 0 /4)
! %f the material is loaded e1ond the 1ield strength#
the material &ill not return to its original shape
after unloading
! %t &ill ha'e some permanent deformation
! %f the material is unloaded at Point 4# the cur'e &ill
proceed from Point 4 to Point 5 $he slope &ill ethe as the slope et&een Point . and 0
! $he distance et&een Point . and 5 indicates the
amount of permanent deformation
5.3 Stress-Strain Diagram (cont)
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• Strain %ardening
! %f the material is loaded again from Point 5# the
cur'e &ill follo& ac" to Point 4 &ith the same
Elastic Modulus(slope)
! $he material no& has a higher 1ield strength of
Point 5
! *aising the 1ield strength 1 permanentl1 straining the material is called Strain Hardening.
5.3 Stress-Strain Diagram (cont)
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• &ensile Strengt' (Point 4)
! $he largest 'alue of stress on the diagram is called
Tensile Strength(TS) or Ultimate Tensile Strength
(UTS)
! %t is the maximum stress &hich the material can
support &ithout rea"ing
• Fra"tre (Point 6)
! %f the material is stretched e1ond Point 4# the stress decreases as nec"ing and non!uniform deformation
occur
! ,racture &ill finall1 occur at Point 6
5.3 Stress-Strain Diagram (cont)
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5. *aterial $ro+erties
• Strength
• +ardness
• Ductilit1
• 7rittleness
• $oughness
Characteristics of Material are descried as
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5. *aterial $ro+erties
1) Strengt'
! Measure of the material propert1 to resist deformation
and to maintain its shape
! %t is 8uantified in terms of 1ield stress or ultimate tensilestrength
! +igh caron steels and metal allo1s ha'e higher strength
than pure metals
! Ceramic also exhiit high strength characteristics
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5. *aterial $ro+erties
2) %ardness ! Measure of the material propert1 to resist indentation#
arasion and &ear
! %t is 8uantified 1 hardness scale such as *oc"&ell and
7rinell hardness scale
! +ardness and Strength correlate &ell ecause oth
properties are related to in!molecular onding
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5. *aterial $ro+erties
3) D"tility
! Measure of the material propert1 to deform efore failure
! %t is 8uantified 1 reading the 'alue of strain at the
fracture point on the stress strain cur'e
! xample of ductile material :
lo& caron steel
aluminum
ule gum
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5. *aterial $ro+erties
) ,rittleness
! Measure of the material9s inabilit to deform efore failure
! $he opposite of ductilit1
! xample of ductile material : glass# high caron steel#
ceramics
D"tile
,rittle
S t r e s
s
Strain
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5. *aterial $ro+erties
5) &og'ness - Measure of the material ailit1 to asor energ
- %t is measured 1 t&o methods
a) %ntegration of stress strain cur'e
! Slo& asorption of energ1
- Asored energ1 per unit 'olume
unit : (l2in) ;(in2in) -l
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5. *aterial $ro+erties
- Charp1 >!Notch $est
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5. *aterial $ro+erties
• Charp1 >!Notch $est (continued)
! $he potential energ1 of the pendulum efore and after
impact can e calculated form the initial and final location
of the pendulum
! $he potential energ1 difference is the energ1 it too" to
rea" the material asored during the impact
! Charp1 test is an impact toughness measurement test
ecause the energ1 is asored 1 the specimen 'er1
rapidl1
" Purpose : to e#aluate the impact toughness as a $unction o$
temperature
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• Charp1 >!Notch $est (continued)
&emperature (6F C h a r p
y & o u g h n e s s (
l b 7 i n
"rittle
"eha8ior
5uctile
"eha8ior
&ransition
&emperature
5. *aterial $ro+erties
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• Charp1 >!Notch $est (continued)
- At lo& temperature# &here the material is rittle and
not strong# little energ1 is re8uired to fracture the material
- At high temperature# &here the material is more ductileand stronger# greater energ1 is re8uired to fracture the
material
-$he transition temperature is the oundar1 et&een rittle
and ductile eha'ior
$he transition temperature is an extremel1 important
parameter in selection of construction material
5. *aterial $ro+erties
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$igh Carbon 3teel
Charpy &est
3tainless 3teel
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) Fatige
5. *aterial $ro+erties
• $he repeated application of stress t1picall1 produced 1
an oscillating load such as 'iration
• Sources of ship 'iration are engine % propeller and &a#es
C1cles N at ,atigue ,ailure
S t r
e s s
( p
s i
) Steel
Alminm
ndurance Limit : A certain threshold
stress &hich &ill not cause the fatigue
failure for the numer of c1cles
Aluminum has no endurance limit
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Fa"tors effe"ting *aterial $ro+erties
5. *aterial $ro+erties
• $emperature :
%ncreasing temperature &ill decrease
! Modulus of lasticit1
! 3ield Strength
! $ensile Strength
Decreasing temperature &ill:
! %ncrease ductilit1
! *educe rittleness• n'ironment
! Sulfites# Chlorine# ?x1gen in &ater# *adiation