lecture02 slides me382 uofm
TRANSCRIPT
-
8/11/2019 Lecture02 Slides ME382 UofM
1/13
ME 382
Lecture 02
Suggested Reading:
A&J-1: 8 (not 8.8); 11.4
-
8/11/2019 Lecture02 Slides ME382 UofM
2/13
3 Important Terms for Mechanical Design
Stiffness
Strength
Toughness
How arethese
different?
-
8/11/2019 Lecture02 Slides ME382 UofM
3/13
Tensile test to measure mechanical properties
lo
P
P
cross sectionalarea Ao
1. Measure length and area
2. Pull specimen
Measure load, P
Measure extension, !
But, this curve depends on your choice of specimen .
-
8/11/2019 Lecture02 Slides ME382 UofM
4/13
Engineering (nominal) stress and strain
Engineering (nominal) stress: !n = P /Ao
(Aois original cross sectional area)
Engineering (nominal) strain: "n = #/ lo(lois original length)
-
8/11/2019 Lecture02 Slides ME382 UofM
5/13
Nominal stress-strain curve for a ductile metal
Nominal stress (MPa)
Nominal strain
X
neckingbegins
(ultimate)
tensile strength
yield strength(yield stress)
(onset of plasticity)
yield begins
linear elastic deformation
(slope =modulus)
plastic deformation
(movement of dislocations)
fracture
-
8/11/2019 Lecture02 Slides ME382 UofM
6/13
Other mechanical properties
Measures of ductility:Percent elongation:
Reduction in area:
100!lf - l0
l0
Energy absorption: U= Pd"#
Energy
per unit volume:u = "nd#n$(area under stress strain curve)
(J)
(Jm-3)
100!A
0- A
break
A0
100!10mm- 5mm
5mm=100%
100!10mm- 7mm
7mm= 42.9%
100!10mm
2- 5mm
2
10mm2
= 50%
100!10mm
2- 7mm
2
10mm2
= 30%
-
8/11/2019 Lecture02 Slides ME382 UofM
7/13
Unloading
Permanent deformation after yield
Note - not the
same slope for
1&2 unless its atrue stress-true
strain curve.
Why?
-
8/11/2019 Lecture02 Slides ME382 UofM
8/13
True Stress and True Strain
After yield, memoryof original shape is lost
$nominal stress and strain may be meaningless
True strain: d"= dl
l
lis current length
True stress: "=P
AAis current area
"="n1+ #
n
( )
"= ln 1+ "
n( )
(if volume is conserved)
-
8/11/2019 Lecture02 Slides ME382 UofM
9/13
Work hardening (strain hardening) results in an increase inyield strength - cold work
Often described by power-lawhardening: "= H#n
True stress / true strain tensile curve
-
8/11/2019 Lecture02 Slides ME382 UofM
10/13
Experimental data for a 5754 aluminum alloy
0
50
100
150
200
250
0 0.05 0.1 0.15 0.2
5754 Aluminum alloy
Truestress(M
Pa)
True strain
"= H#n
-
8/11/2019 Lecture02 Slides ME382 UofM
11/13
1
10
100
1000
0.001 0.01 0.1
5754 Aluminum alloy
Truestress(MP
a)
True strain
!= 367 "0.238~ ~
Determining the strain-hardening parameters
!! = H!!n
ln !! = n ln!!+ lnH
-
8/11/2019 Lecture02 Slides ME382 UofM
12/13
0
50
100
150
200
250
0 0.02 0.04 0.06 0.08 0.1
5754 Aluminum alloy
Truestress(MP
a)
True strain
power law
experimental data
Comparison of power-law with experimental results
Pretty good!
-
8/11/2019 Lecture02 Slides ME382 UofM
13/13
There are other forms of uniaxial stress-strain curves.