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Exam 1 Solutions - Introduction to the Science of Engineering Materials | MATS 2001, Exams of Materials science

Material Type: Exam; Professor: Schott; Class: Introduction to the Science of Engineering Materials; Subject: Materials Science; University: University of Minnesota - Twin Cities; Term: Fall 2012;

Typology: Exams

2012/2013

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MatS 2001 - Exam #1 Solution
Question 1 True/False (15 Points)
Red answers are correct.
a) T F The strain hardening exponent in the relationship

TK
T
n
is equal
to the true strain at the point where necking begins.
b) T F A stiff material has a low modulus of elasticity.
c) T F Poisson’sratioisbasedonconstantvolumeintheelasticregion
d) T F If Internal and surface cracks are initially the same size, the internal
crack will cause fatigue failure before the external crack.
e) T F The Larson Miller Parameter directly relates creep failure time to
applied stress.
f) T F Typical yield stresses for metals are in the range of 10-300 GPa.
g) T F Themostimportantfactorindeterminingamaterial’sresistanceto
fracture is the number of cracks in it.
h) T F Crack growth rate in fatigue decreases as the crack length
increases.
i) T F Ceramics have higher KIC values than metals.
j) T F KIC is small for metals because they have some ductility.
k) T F Plastic deformation results in a permanent change in shape.
l) T F Crack propagation in brittle failure becomes easier as the crack
length increases.
m) T F Fracture can happen before the yield stress is reached.
n) T F For a brittle material, yield stress and tensile strength can be the
same
o) T F True stress is always smaller than Engineering stress.
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MatS 2001 - Exam # 1 Solution

Question 1 True/False (15 Points)

Red answers are correct.

a) T F The strain hardening exponent in the relationship

T

 K 

T

n

is equal

to the true strain at the point where necking begins.

b) T F A stiff material has a low modulus of elasticity.

c) T F Poisson’s ratio is based on constant volume in the elastic region

d) T F If Internal and surface cracks are initially the same size, the internal

crack will cause fatigue failure before the external crack.

e) T F The Larson – Miller Parameter directly relates creep failure time to

applied stress.

f) T F Typical yield stresses for metals are in the range of 10-300 GPa.

g) T F The most important factor in determining a material’s resistance to

fracture is the number of cracks in it.

h) T F Crack growth rate in fatigue decreases as the crack length

increases.

i) T F Ceramics have higher K IC

values than metals.

j) T F K IC

is small for metals because they have some ductility.

k) T F Plastic deformation results in a permanent change in shape.

l) T F Crack propagation in brittle failure becomes easier as the crack

length increases.

m) T F Fracture can happen before the yield stress is reached.

n) T F For a brittle material, yield stress and tensile strength can be the

same

o) T F True stress is always smaller than Engineering stress.

Question 2 Creep (15 Points)

The hook shown to the right will support a container of molten steel and must carry a load of

40,000 lb. The hook operates continuously at a temperature of 5 83 C. The relationship

between stress and Larson – Miller parameter is shown below:

3

L-M T 38.316 1.796log 10 day

t x

  when T is in Kelvin and rupture time is in days. Note:

“log” is common log, base 10.

a) If the useful life of the hook, with a safety factor of 2, is to be 10 years of

continuous operation, what must be the diameter (in inches) of the indicated

portion of the hook? (10 pts)

3

2 2

L-M 583+273 38.316 1.796 log 3650 10 38.

From graph stress 2,000 psi, or with safety factor,

design stress = 1,000 psi

, or 40 in , 40 50.

1,000 psi

7.14 in.

x

F lb

A d

d

Question 4 Stress/Strain Curve ( 20 points)

Consider the stress-strain curve below for a metal alloy.

(a) Calculate the elastic modulus, (in GPa), the yield stress, yield strain, tensile

strength, and strain at necking. Show your work on the graph. (10 pts)

..

 

200 MPa 0 MPa

E

0 0

80

025 0 0

GPa

Yield stress is found using a line with slope = E and 0.2% offset.

As shown on the graph: y = 250 MPa

Yield strain can be read directly from the graph:  y

= 0.

As an alternative, .

,

   . y

250 MPa

0 002

80 000 M a

0

P

005

Tensile strength is the maximum of the curve = 450 MPa

Strain at necking is strain at tensile strength = 0.

(b) A 2 m long, 2mm diameter rod of this alloy is loaded with 1 28 kg. What are the

resulting stress, strain, length, and diameter of the rod while loaded? When the load is

removed, what is the length of the rod? (1 0 pts)

With 1 28 kg.,

2 2

(128 kg)(9.81 m)(4)

399.3 MPa

(2 mm) s

From the graph:  total

= 0.

0

l  l ( 1  ) ( .2 0 m)(1+0.125) = 2.25 m

2

2

0 0

0 0

2

mm 2 m

, or , or , D=1.89 mm

4 2.25 m

or

1 399.3 MPa 1.125 450 MPA

A 2.79 mm , D 1.88 mm

i

i i i

i

T

i i

T

A l D

Al A l A

l

F

plastic 0 plastic

plastic total elastic plastic

400 MPa

80 GPa

l l (1 ) (2.0 m)(1 0.120) 2.24 m

or  

      

(b) True stress and strain

Portion of the graph up to necking will be about the same as the engineering stress-

strain graph. The strain scale will expand as calculated below, and the true stress at

failure will be double the engineering stress at failure since the necking area is ½ the

original area.

Justify your strain axis in (b) by an appropriate calculation. (5 pts)

Beyond the onset of necking, true strain must be calculated by area ratio. At fracture, the area

is ½ the original area.

0

0

ln ln ln(2) 0.

i

T

i

l A

l A

0

1

2

3

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.