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Practice Midterm 02 Solutions 2000<br />
Question 1 (30 points)<br />
<strong>Use</strong> <strong>the</strong> <strong>grid</strong> <strong>below</strong> <strong>to</strong> <strong>draw</strong> <strong>the</strong> <strong>Al</strong>-<strong>Li</strong> <strong>phase</strong> <strong>diagram</strong> <strong>based</strong> <strong>upon</strong> <strong>the</strong> following<br />
experimental observations (all compositions in weight %). Label all <strong>phase</strong> fields.<br />
T(°C)<br />
800<br />
600<br />
400<br />
200<br />
Pure <strong>Al</strong> melts at 660°C; pure <strong>Li</strong> melts at 181°C. At 600°C, liquid of 10 %<strong>Li</strong> solidifies <strong>to</strong><br />
form α <strong>phase</strong> of 4 %<strong>Li</strong> and δ <strong>phase</strong> of 20 %<strong>Li</strong>. Pure δ <strong>phase</strong> containing 20 %<strong>Li</strong> melts<br />
congruently at 718°C. At 521°C, γ <strong>phase</strong> containing 34 %<strong>Li</strong> melts <strong>to</strong> form δ <strong>phase</strong> of 24<br />
%<strong>Li</strong> and liquid <strong>phase</strong> of 47 %<strong>Li</strong>. At 620°C, a 30 % <strong>Li</strong> alloy has equal parts of liquid<br />
<strong>phase</strong> and δ <strong>phase</strong>, while at 260°C, a 60 %<strong>Li</strong> alloy has equal parts of liquid <strong>phase</strong> and γ<br />
<strong>phase</strong>. At 179°C, liquid containing 98 %<strong>Li</strong> solidifies <strong>to</strong> form γ <strong>phase</strong> (34 %<strong>Li</strong>) and β<br />
<strong>phase</strong> (99 %<strong>Li</strong>). At 0°C, <strong>Al</strong> can dissolve up <strong>to</strong> 3 % <strong>Li</strong>, while <strong>Li</strong> can dissolve no more than<br />
0.5 % <strong>Al</strong>; however. <strong>Al</strong>so at 0°C, <strong>the</strong> solubility of <strong>Li</strong> in <strong>the</strong> δ <strong>phase</strong> ranges from 20 <strong>to</strong> 22<br />
%<strong>Li</strong>.<br />
α +L<br />
α<br />
α + δ<br />
L+δ<br />
δ<br />
δ +L<br />
γ<br />
<strong>Li</strong>quid<br />
δ + γ L+β<br />
β<br />
<strong>Al</strong> 20 40 60 80<br />
<strong>Li</strong><br />
wt% <strong>Li</strong><br />
γ +L<br />
γ + β<br />
page 1 of 8
Question 2 (20 points)<br />
T(°C)<br />
800<br />
0.02<br />
600<br />
α<br />
400<br />
(ferrite)<br />
200<br />
Practice Midterm 02 Solutions 2000<br />
Illustrate <strong>the</strong> microstructural evolution resulting from cooling a hypereutec<strong>to</strong>id AISI<br />
1095 steel through <strong>the</strong> eutec<strong>to</strong>id decomposition iso<strong>the</strong>rm. <strong>Use</strong> <strong>the</strong> templates at right,<br />
which show <strong>the</strong> prior austenite grains, and accurately <strong>draw</strong> <strong>the</strong> equilibrium<br />
microstructures at each of <strong>the</strong> temperatures identified on <strong>the</strong> right. Label each <strong>phase</strong>,<br />
and label all relevant microstructural constituents by <strong>the</strong>ir common metallurgical<br />
names.<br />
1600<br />
1538°<br />
1495°<br />
δ<br />
1400<br />
1394°<br />
1200<br />
γ<br />
(austenite)<br />
1000<br />
0.77<br />
γ +<br />
2.1<br />
1148°<br />
α +<br />
727°<br />
4.3<br />
Fe 1 2 3 4 5 6 7<br />
wt% C<br />
L<br />
γ +<br />
L+<br />
6.7<br />
Fe3<br />
(cementite)<br />
Austenite<br />
1150°C<br />
100% Austenite<br />
Proeutec<strong>to</strong>id cementite<br />
at grain boundaries<br />
750°C<br />
92% austenite; 8% cementite<br />
Proeutec<strong>to</strong>id cementite<br />
Pearlite<br />
450°C<br />
86% ferrite; 14%<br />
cementite<br />
Proeutec<strong>to</strong>id cementite<br />
Pearlite<br />
25°C<br />
86% ferrite; 14% cementite<br />
page 2 of 8
Question 3 (30 points)<br />
Sketch and label <strong>the</strong> iso<strong>the</strong>rmal cooling curves for <strong>the</strong> same AISI 1095 steel that<br />
produce <strong>the</strong> following microstructures: Note that <strong>the</strong>re are three TTT curves here.<br />
Label <strong>the</strong> first with a) and b), <strong>the</strong> second with c) and d), and <strong>the</strong> third with e) and f).<br />
a) 100% martensite<br />
b) 5% proeuctec<strong>to</strong>id cementite and 95% martensite<br />
T (°C)<br />
800<br />
700<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
840°<br />
727°<br />
Ms<br />
M90<br />
1 sec<br />
γ + Fe3C<br />
α + Fe3C<br />
1 min 1 hour<br />
1 day<br />
0.1 1 10 102 103 104 105 0<br />
(a) (b)<br />
Time (sec)<br />
Practice Midterm 02 Solutions 2000<br />
page 3 of 8
c) 25% coarse pearlite, 75% martensite<br />
d) 100% fine pearlite<br />
T (°C)<br />
800<br />
700<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
840°<br />
727°<br />
Ms<br />
M90<br />
1 sec<br />
γ + Fe3C<br />
α + Fe3C<br />
1 min 1 hour<br />
1 day<br />
0.1 1 10 102 103 104 105 0<br />
Time (sec)<br />
(c) (d)<br />
Practice Midterm 02 Solutions 2000<br />
page 4 of 8
e) 25% upper bainite and 75% tempered martensite<br />
f) 25% fine pearlite, 25% lower bainite, 50% martensite<br />
T (°C)<br />
800<br />
700<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
840°<br />
727°<br />
Ms<br />
M90<br />
1 sec<br />
γ + Fe3C<br />
α + Fe3C<br />
1 min 1 hour<br />
1 day<br />
0.1 1 10 102 103 104 105 0<br />
Time (sec)<br />
(f)<br />
(e)<br />
Practice Midterm 02 Solutions 2000<br />
page 5 of 8
Question 4 (20 points)<br />
Mark <strong>the</strong> checkbox next <strong>to</strong> <strong>the</strong> best answer (only one) in each case.<br />
a) Martensite is a metastable <strong>phase</strong> produced in ferrous alloys by<br />
holding at a specific temperature for a specific time<br />
heating <strong>to</strong> a specific temperature over a specific time<br />
☒ cooling <strong>to</strong> a specific temperature over a specific time<br />
b) Martensite can be tempered by<br />
heating <strong>to</strong> a specific temperature over a specific time<br />
cooling <strong>to</strong> a specific temperature over a specific time<br />
☒ holding at a specific temperature for a specific time<br />
c) The microstructure of tempered martensite consists of<br />
pearlite and bainite<br />
only bainite<br />
☒ nei<strong>the</strong>r pearlite nor bainite<br />
d) Martensite is strong because<br />
it is not an equilibrium <strong>phase</strong><br />
☒ it presents many obstacles <strong>to</strong> dislocation motion<br />
it is a highly dis<strong>to</strong>rted arrangement of Fe and C a<strong>to</strong>ms<br />
e) Ferrous alloys can be precipitation-hardened by<br />
holding in <strong>the</strong> austenite+ferrite two-<strong>phase</strong> field<br />
☒ aging <strong>to</strong> produce alloy carbides<br />
quenching <strong>to</strong> produce martensite<br />
f) Nonferrous metallic alloys can be precipitation-hardened by<br />
☒ solutionizing, quenching and aging<br />
solutionizing slow-cooling and quenching<br />
quenching, aging and quenching<br />
g) Ni-base superalloys are known for <strong>the</strong>ir superior<br />
☒ strength at elevated temperatures<br />
<strong>to</strong>ughness at room temperature<br />
wear-resistant surface finish<br />
Practice Midterm 02 Solutions 2000<br />
page 6 of 8
h) <strong>Al</strong>-base alloys are protected from oxidation by<br />
☒ a passivating oxide film<br />
a high density of second <strong>phase</strong> particles<br />
an ASTM standard requiring painted surfaces<br />
i) During annealing, <strong>the</strong> driving force for <strong>the</strong> recovery stage is<br />
☒ reduction in strain energy<br />
reduction in surface energy<br />
reduction in chemical potential<br />
j) During annealing, <strong>the</strong> driving force for <strong>the</strong> recrystallization stage is<br />
☒ reduction in strain energy<br />
reduction in surface energy<br />
reduction in chemical potential<br />
k) During annealing, <strong>the</strong> driving force for <strong>the</strong> grain growth stage is<br />
reduction in strain energy<br />
☒ reduction in surface energy<br />
reduction in chemical potential<br />
l) Ceramics are often formed in<strong>to</strong> complex parts by sintering at<br />
one-forth of <strong>the</strong> melting temperature<br />
☒ one-third of <strong>the</strong> melting temperature<br />
two-thirds of <strong>the</strong> melting temperature<br />
m) Glass-ceramics are subjected <strong>to</strong> an aging treatment in order <strong>to</strong><br />
provide stress-relief<br />
remove surface cracks<br />
☒ precipitate a crystalline <strong>phase</strong><br />
n) The most significant attribute associated with a Griffith crack is<br />
its location at <strong>the</strong> surface<br />
its length<br />
☒ its tip radius<br />
Practice Midterm 02 Solutions 2000<br />
page 7 of 8
o) Addition polymerization is a reaction among small organic molecules involving<br />
isotropic growth<br />
☒ chain growth<br />
step growth<br />
p) Condensation polymerization involves<br />
a rapid “chain reaction”<br />
☒ individual chemical reactions between pairs of reactive monomers<br />
electron transport in <strong>the</strong> condensate<br />
q) The primary role of <strong>the</strong> initia<strong>to</strong>r in a polymerization reaction is <strong>to</strong><br />
begin <strong>the</strong> assembly of mers in<strong>to</strong> chains<br />
☒ convert double bonds in<strong>to</strong> single bonds<br />
nucleate <strong>the</strong> condensation reaction<br />
r) <strong>Li</strong>near polymers are <strong>the</strong> result of bonding between<br />
☒ bifunctional mers<br />
polyfunctional mers<br />
linear mers<br />
s) A block co-polymer can also be described as<br />
a solid solution<br />
☒ a two <strong>phase</strong> alloy<br />
a cubic crystal structure<br />
t) A polymer is described as “viscoelastic” when it shows<br />
☒ slow recovery of strain<br />
viscous fracture<br />
negative modulus of elasticity<br />
Practice Midterm 02 Solutions 2000<br />
page 8 of 8
UNIVERSITY OF CALIFORNIA<br />
College of Engineering<br />
Department of Materials Science and Engineering<br />
Professor R. Gronsky Fall Semester 2001<br />
ENGINEERING 45
E45•Midterm #2<br />
Question 1 The silver-mercury system forms <strong>the</strong> basis of an important biomaterial<br />
known as dental amalgam, which has been used for decades in res<strong>to</strong>rative<br />
dental fillings. The term “amalgam” is frequently used <strong>to</strong> depict many<br />
different alloys of mercury, originating from <strong>the</strong> “amalgamation” process <strong>to</strong><br />
refine ores of <strong>the</strong> precious metals, primarily silver and gold. The finely<br />
crushed ores in aqueous solution are mixed with mercury, allowing <strong>the</strong><br />
mercury <strong>to</strong> alloy with <strong>the</strong> precious metals, forming an amalgam. When <strong>the</strong><br />
amalgam is heated, <strong>the</strong> mercury is driven off as a vapor (collected and<br />
recycled of course), leaving behind pure precious metal “sponge.”<br />
1000<br />
961.93°<br />
800<br />
600<br />
T<br />
(°C)<br />
400<br />
Silver (Ag, Z = 47) is fcc and melts at 961.93°C, mercury (Hg, Z = 80)<br />
freezes at –38.862°C. The equilibrium β <strong>phase</strong> has AgHg s<strong>to</strong>ichiometry and<br />
an hcp Bravais lattice. The equilibrium γ <strong>phase</strong> has Ag2Hg3 s<strong>to</strong>ichiometry and<br />
a bcc Bravais Lattice.<br />
<strong>Use</strong> this information and <strong>the</strong> equilibrium <strong>phase</strong> <strong>diagram</strong> for <strong>the</strong> silver-mercury<br />
binary system due <strong>to</strong> M. Hanson (Constitution of Binary <strong>Al</strong>loys, 2 nd . Edition,<br />
McGraw –Hill, 1958) shown <strong>below</strong> <strong>to</strong> choose <strong>the</strong> best answers for 2 points<br />
each.<br />
(Ag)<br />
200<br />
127°<br />
β<br />
0<br />
γ<br />
-38.9°<br />
-38.862°<br />
(Hg)<br />
-200<br />
Ag 10 20 30 40 50 60 70 80 90 Hg<br />
Weight Percentage Hg<br />
2 of 10<br />
52.4<br />
L<br />
276°<br />
Hg Boiling Point 357°
E45•Midterm #2<br />
a. The number of components in this binary system is<br />
one (1)<br />
two (2)<br />
three (3)<br />
b. The <strong>phase</strong> called (Ag) is actually<br />
pure silver<br />
a silver-mercury solid solution<br />
a metastable <strong>phase</strong><br />
c. Based <strong>upon</strong> <strong>the</strong> Gibbs Phase Rule (P+F = C+2), <strong>the</strong> number of degrees of<br />
freedom available <strong>to</strong> pure Hg at 357°C in this system is<br />
zero (0)<br />
one (1)<br />
two (2)<br />
d. The number of degrees of freedom available <strong>to</strong> a 40 wt.% Ag alloy at 276°C is<br />
zero (0)<br />
one (1)<br />
two (2)<br />
e. The maximum solubility of mercury in silver is<br />
infinitesimally small<br />
undefined because mercury is a liquid at room temperature<br />
established by <strong>the</strong> highest temperature reaction iso<strong>the</strong>rm<br />
f. Both β <strong>phase</strong> and γ <strong>phase</strong> are in equilibrium with liquid Hg at a<br />
monotectic<br />
eutectic<br />
peritectic<br />
g. When β <strong>phase</strong> of 60 wt% Hg melts, it<br />
disappears completely<br />
passes through a β + L two-<strong>phase</strong> equilibrium<br />
generates mercury vapor<br />
h. A dental hygienist “mixes” amalgam immediately before <strong>the</strong> dentist applies it so<br />
that it will “harden” as a complete filling. The hardening process is due <strong>to</strong><br />
solid state diffusion<br />
solidification of liquid Hg<br />
dislocations created during mixing<br />
i. An amalgam of 20 wt % Hg in equilibrium will decompose when heated above<br />
276°C<br />
576 °C<br />
776°C<br />
j. Dental fillings made of silver amalgam are at risk of leaking mercury in<strong>to</strong> <strong>the</strong><br />
mouth if <strong>the</strong> equilibrium mercury concentration exceeds<br />
52.4%<br />
62.4%<br />
72.4%<br />
3 of 10
E45•Midterm #2<br />
Question 2 <strong>Use</strong> <strong>the</strong> same <strong>phase</strong> <strong>diagram</strong> <strong>to</strong> now sketch <strong>the</strong> microstructures expected<br />
during equilibrium solidification of <strong>the</strong> following alloys. The lever rule<br />
construction is important here. Draw a vertical line on <strong>the</strong> <strong>phase</strong> <strong>diagram</strong> for<br />
<strong>the</strong> specified composition and show all tie lines used <strong>to</strong> establish your<br />
equilibrium microstructures. Remember that <strong>the</strong> high temperature<br />
microstructure influences <strong>the</strong> lower temperature microstructure. Clearly label<br />
all <strong>phase</strong>s for full credit.<br />
T = 500°C<br />
85% (Ag)<br />
+ 15% L<br />
T = 25°C<br />
40% (Ag)<br />
+ 60% β<br />
T = 200°C<br />
50% L<br />
+ 50% β<br />
T = 25°C<br />
33% L<br />
+ 67% γ<br />
Each sketch is worth 5 points.<br />
a. Ag-55 wt% Hg<br />
L<br />
(Ag)<br />
b. Hg-20 wt% Ag<br />
β L<br />
γ L<br />
(Ag)<br />
1000<br />
961.93°<br />
800<br />
600<br />
T<br />
(°C)<br />
400<br />
200<br />
127°<br />
β<br />
0<br />
-38.862°<br />
-38.9°<br />
γ<br />
(Hg)<br />
-200<br />
Ag 10 20 30 40 50 60 70 80 90 Hg<br />
Weight Percentage Hg<br />
1000<br />
961.93°<br />
800<br />
600<br />
T<br />
(°C)<br />
400<br />
Note that in all cases here, <strong>the</strong>re are no microstructural remnants from higher<br />
temperature reactions <strong>to</strong> influence <strong>the</strong> products. <strong>Al</strong>l are peritectic reactions, which<br />
require longer times <strong>to</strong> reach equilibrium, but time is not a fac<strong>to</strong>r here since we are<br />
working from an equilibrium <strong>phase</strong> <strong>diagram</strong>.<br />
4 of 10<br />
(Ag)<br />
(Ag)<br />
52.4<br />
52.4<br />
L<br />
276°<br />
Hg Boiling Point 357°<br />
200<br />
127°<br />
β<br />
0<br />
-38.862°<br />
-38.9°<br />
γ<br />
(Hg)<br />
-200<br />
Ag 10 20 30 40 50 60 70 80 90 Hg<br />
Weight Percentage Hg<br />
L<br />
276°<br />
Hg Boiling Point 357°
E45•Midterm #2<br />
Question 3 The same TTT curve for a plain carbon steel of eutec<strong>to</strong>id composition is<br />
reproduced multiple times <strong>below</strong>. Draw directly on <strong>the</strong>se plots <strong>the</strong> cooling<br />
curves corresponding <strong>to</strong> <strong>the</strong> specified treatments. Remember that TTT curves<br />
are appropriate for iso<strong>the</strong>rmal transformations only. The actual start and<br />
termination of <strong>the</strong> decomposition of austenite during continuous cooling<br />
occurs at slightly lower temperatures and longer times than shown here.<br />
Each curve is worth 5 points.<br />
a. Austempering, a commercial<br />
treatment used <strong>to</strong> avoid quench<br />
cracking. Show and label <strong>the</strong><br />
curves corresponding <strong>to</strong> both<br />
<strong>the</strong> surface and <strong>the</strong> interior of a<br />
thick cross section steel beam.<br />
b. Martempering, a commercial<br />
treatment used <strong>to</strong> avoid quench<br />
cracking. Show and label <strong>the</strong><br />
curves corresponding <strong>to</strong> both<br />
<strong>the</strong> surface and <strong>the</strong> interior of a<br />
thick cross section steel beam.<br />
Both (a) and (b) are <strong>the</strong> classic, traditional methods used widely throughout <strong>the</strong><br />
engineering community <strong>to</strong> prevent quench-cracking in large cross-section steel<br />
components.<br />
5 of 10<br />
°C<br />
800<br />
700<br />
600<br />
500<br />
727°<br />
γ<br />
γ<br />
α + Fe 3 C<br />
400<br />
upper bainite<br />
Surface Interior<br />
300<br />
215°<br />
200<br />
Transform<br />
lower<br />
bainite<br />
100<br />
martensite<br />
sec min<br />
Quench<br />
hour day<br />
°C<br />
800<br />
700<br />
600<br />
500<br />
0.1 1 10 10 2 10 3 10 4 10 5<br />
727°<br />
γ<br />
γ<br />
time (sec)<br />
α + Fe 3 C<br />
coarse pearlite<br />
fine pearlite<br />
400<br />
upper Temper bainite<br />
Surface Interior<br />
300<br />
215°<br />
200<br />
martensite<br />
100 sec<br />
Quench<br />
min hour<br />
lower<br />
bainite<br />
day<br />
0.1 1 10 10 2 10 3 10 4 10 5<br />
time (sec)<br />
coarse pearlite<br />
fine pearlite
E45•Midterm #2<br />
c. An “interrupted quench”<br />
technique that would generate a<br />
final microstructure of 50%<br />
lower bainite and 50% fine<br />
pearlite. In this case <strong>the</strong><br />
workpiece is a small diameter<br />
rod <strong>to</strong> be used as an axle in a<br />
mo<strong>to</strong>r-genera<strong>to</strong>r set.<br />
The only way this treatment can be an “interrupted quench” is <strong>to</strong> begin with <strong>the</strong> high<br />
temperature transformation (fine pearlite), holding iso<strong>the</strong>rmally until <strong>the</strong> reaction<br />
progresses half way between <strong>the</strong> start and finish lines. Note that this amounts <strong>to</strong><br />
only a few seconds. The untransformed austenite is <strong>the</strong>n lowered in temperature<br />
and held iso<strong>the</strong>rmally until it fully transforms <strong>to</strong> lower bainite as shown.<br />
d. An approximation. Show<br />
without compensation for<br />
continuous cooling <strong>the</strong> T-t<br />
trajec<strong>to</strong>ry for a sample that was<br />
left in <strong>the</strong> furnace during a<br />
power outage. The initial<br />
temperature was 800°C at<br />
midnight when <strong>the</strong> power failed.<br />
The cooling rate for <strong>the</strong> wellinsulated<br />
furnace was previously<br />
calibrated at 100°C / minute.<br />
The sample was recovered 8<br />
hours later at <strong>the</strong> start of <strong>the</strong><br />
daylight shift.<br />
In question (d), note that a linear rate of 100°C / min is dramatically curved on <strong>the</strong><br />
log scale used here. <strong>Al</strong>though this is only an “approximation” because <strong>the</strong> cooling<br />
treatment is not iso<strong>the</strong>rmal, it is reasonable <strong>to</strong> expect that <strong>the</strong> final microstructure<br />
would be fully pearlitic, and ra<strong>the</strong>r coarse.<br />
6 of 10<br />
°C<br />
800<br />
700<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
°C<br />
800<br />
700<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
727°<br />
γ<br />
215°<br />
γ<br />
α + Fe 3 C<br />
martensite<br />
sec min hour day<br />
0.1 1 10 10 2 10 3 10 4 10 5<br />
727°<br />
γ<br />
215°<br />
50%<br />
γ<br />
time (sec)<br />
coarse pearlite<br />
fine pearlite<br />
upper bainite<br />
lower<br />
remaining 50%<br />
bainite<br />
100°C/min<br />
coarse pearlite<br />
α + Fe3C fine pearlite<br />
martensite<br />
sec min hour day<br />
0.1 1 10 10 2 10 3 10 4 10 5<br />
time (sec)<br />
upper bainite<br />
lower<br />
bainite
E45•Midterm #2<br />
Question 4 Pure zirconia undergoes an allotropic transformation at 1000°C from a high<br />
temperature tetragonal structure <strong>to</strong> a low temperature monoclinic structure.<br />
A massive volume expansion <strong>upon</strong> cooling through <strong>the</strong> tetragonal-<strong>to</strong>monoclinic<br />
transformation literally results in <strong>the</strong> self destruction of <strong>the</strong> crystal.<br />
Thermal cycling through <strong>the</strong> transformation temperature pulverizes <strong>the</strong><br />
material in<strong>to</strong> a fine powder.<br />
However, alloying zirconia with 25 mol % calcia yields a cubic <strong>phase</strong> that<br />
persists up <strong>to</strong> its melting point with no structural instabilities. This<br />
“stabilized” zirconia is a very popular structural ceramic for that reason.<br />
T<br />
(°C)<br />
2500<br />
2000<br />
Tetragonal<br />
ZrO2 SS<br />
1500<br />
1000<br />
Monoclinic<br />
ZrO2 SS<br />
500<br />
ZrO 2<br />
10<br />
Cubic<br />
ZrO 2 SS<br />
20 30 40 50<br />
Mole Percentage CaO<br />
a. Using this information, explain how “partially-stabilized” zirconia, which<br />
contains some cubic, some tetragonal, and some monoclinic <strong>phase</strong>s, is<br />
prepared. Be specific, using <strong>the</strong> equilibrium <strong>phase</strong> <strong>diagram</strong> above and your<br />
understanding of <strong>phase</strong> transformation kinetics for 10 points.<br />
The <strong>phase</strong> <strong>diagram</strong> indicates that it is not possible <strong>to</strong> find all three <strong>phase</strong>s (cubic,<br />
tetragonal and monoclinic) in equilibrium. So this is a problem involving kinetics. At<br />
CaO concentrations less than 15 mol%, monoclinic and cubic <strong>phase</strong>s are in equilibrium<br />
at room temperature. To include a tetragonal <strong>phase</strong> at room temperature, all that is<br />
required is <strong>to</strong> heat above <strong>the</strong> eutec<strong>to</strong>id temperature (900°C) where tetragonal<br />
<strong>phase</strong> is in equilibrium, <strong>the</strong>n “quench” <strong>to</strong> retain it kinetically at lower temperature.<br />
7 of 10<br />
L<br />
ZrCaO 3
E45•Midterm #2<br />
b. For ano<strong>the</strong>r 10 points, explain in detail how <strong>the</strong> partially-stabilized zirconia<br />
structure leads <strong>to</strong> “transformation <strong>to</strong>ughening” of an o<strong>the</strong>rwise brittle ceramic<br />
material. Comment specifically on <strong>the</strong> volume expansion associated with <strong>the</strong><br />
tetragonal <strong>to</strong> monoclinic transformation, and its role in causing an increase in<br />
fracture <strong>to</strong>ughness. Recall that fracture <strong>to</strong>ughness refers <strong>to</strong> <strong>the</strong> performance<br />
of a material with pre-existing flaws, and focus your attention on <strong>the</strong> crack<br />
shown in <strong>the</strong> following sketch.<br />
Recalling from above that only <strong>the</strong> cubic<br />
and monoclinic <strong>phase</strong>s are in equilibrium<br />
at room temperature, <strong>the</strong> metastable<br />
tetragonal <strong>phase</strong> becomes <strong>the</strong> key<br />
constituent in this problem.<br />
As <strong>the</strong> crack advances through <strong>the</strong><br />
forest of tetragonal precipitates, it<br />
relaxes <strong>the</strong> constraints of <strong>the</strong> cubic<br />
monoclinic<br />
matrix confining <strong>the</strong> tetragonal<br />
particles. This relaxation induces <strong>the</strong><br />
cubic matrix<br />
transformation of <strong>the</strong> metastable<br />
tetragonal <strong>phase</strong> <strong>to</strong> <strong>the</strong> equilibrium<br />
monoclinic <strong>phase</strong> in <strong>the</strong> vicinity of <strong>the</strong><br />
crack tip. The resulting volume<br />
expansion (as described in <strong>the</strong> problem<br />
statement) exerts a closing force on<br />
<strong>the</strong> crack tip, retarding its progress<br />
through <strong>the</strong> ceramic. It is for this reason that <strong>the</strong> mechanism described here is<br />
known as “transformation <strong>to</strong>ughening.” The transformation from <strong>the</strong> tetragonal <strong>to</strong><br />
monoclinic <strong>phase</strong>s gives partially stabilized zirconia (PSZ) <strong>the</strong> highest fracture<br />
<strong>to</strong>ugnhness of all structural ceramics.<br />
8 of 10<br />
tetragonal
E45•Midterm #2<br />
Question 5 Polymers or “many mers” may result from chain growth, also known as<br />
addition polymerization, which generates linear or branched polymers, or<br />
from step growth, also known as condensation polymerization, which<br />
generates network polymers. The mechanical properties of polymers are, like<br />
all materials, linked <strong>to</strong> <strong>the</strong>ir structure.<br />
(a) The styrene mer is shown schematically <strong>below</strong>. Show how polystyrene results<br />
from a polymerization reaction by sketching <strong>the</strong> final product containing at<br />
least five mers. Is polystyrene a (check all that apply)<br />
linear,<br />
branched, or<br />
network polymer?<br />
Showing <strong>the</strong> correct polymeric structure and checking <strong>the</strong> correct box(es)<br />
above earns 10 points.<br />
The signature feature of <strong>the</strong> styrene mer that marks it as a candidate for<br />
polymerization is its double carbon bond. Conversion of this bond in<strong>to</strong> two single<br />
bonds functionalizes <strong>the</strong> mer. Its resulting bifunctional character makes it a<br />
candidate for chain growth in<strong>to</strong> a linear polymer, just like polyethylene. A segment<br />
of <strong>the</strong> polymer backbone chain is shown <strong>below</strong>.<br />
H H<br />
C C<br />
H<br />
H C CH 2<br />
This particular configuration is <strong>the</strong> isotactic one, with all of <strong>the</strong> large side groups on<br />
<strong>the</strong> same side. The syndiotactic configuration shown <strong>below</strong>, and <strong>the</strong> atactic<br />
configuration (random) are also acceptable.<br />
H H<br />
C C<br />
H<br />
H H<br />
C C<br />
H<br />
H<br />
H<br />
C C<br />
H<br />
9 of 10<br />
H H<br />
C C<br />
H<br />
H H<br />
C C<br />
H<br />
H H<br />
C C<br />
H<br />
H<br />
H<br />
C C<br />
H<br />
H H<br />
C C<br />
H<br />
H H<br />
C C<br />
H
E45•Midterm #2<br />
(b) Polymers, like metals and ceramics, can be described by a lattice and motif,<br />
but <strong>the</strong>y are never fully crystalline. In fact, numerous polymers are<br />
completely amorphous. Those that possess some crystallinity have <strong>the</strong>ir<br />
polymeric chains arranged in a regular, parallel alignment, and <strong>the</strong>se<br />
crystallites or “fringed micelles” are embedded in an amorphous matrix.<br />
A partially crystallized <strong>the</strong>rmoplastic polymer shows “viscoelastic” mechanical<br />
behavior. Using <strong>the</strong> coordinate axes <strong>below</strong>, plot <strong>the</strong> elastic modulus as a<br />
function of temperature for a viscoelastic polymer. Note particularly <strong>the</strong><br />
changes seen at <strong>the</strong> glass transition temperature and <strong>the</strong> melting<br />
temperature. On your plot, label <strong>the</strong> four distinct regions of behavior<br />
associated with viscoelasticity, that is, rubbery, viscous, lea<strong>the</strong>ry, and rigid<br />
(or elastic). A correctly labeled plot is worth 10 points.<br />
Modulus<br />
of<br />
Elasticity<br />
(log scale)<br />
T g<br />
Temperature<br />
In its traditional definition, <strong>the</strong> glass transition temperature marks <strong>the</strong> transition<br />
from rigid “crystal-like” <strong>to</strong> viscous “glass-like” mechanical behavior. Crystals deform<br />
by dislocation motion, glasses deform by <strong>the</strong> viscous flow.<br />
At <strong>the</strong> melting point, viscous flow is most obvious because <strong>the</strong> material cannot<br />
sustain its own weight against gravity. The elastic modulus drops <strong>to</strong> zero.<br />
10 of 10<br />
Rigid (or "Elastic")<br />
T m<br />
Lea<strong>the</strong>ry<br />
Rubbery<br />
Viscous
UNIVERSITY OF CALIFORNIA<br />
College of Engineering<br />
Department of Materials Science & Engineering<br />
Professor R. Gronsky Fall Semester, 2005<br />
Engineering 45 Midterm 02<br />
SOLUTIONS<br />
INSTRUCTIONS<br />
LATTICE seating .................. Please be seated with occupied seats <strong>to</strong> your front and back, vacant seats <strong>to</strong> your left and right.<br />
CLOSED BOOK format ...... <strong>Al</strong>l you need are writing instruments and a straightedge. Please s<strong>to</strong>re all books, reference materials,<br />
calcula<strong>to</strong>rs, PDAs, cell phones (OFF), and iPods.<br />
NO DISRUPTION rule ......... Questions cause <strong>to</strong>o much of a disturbance <strong>to</strong> o<strong>the</strong>rs in <strong>the</strong> room. Instead of asking questions,<br />
write any concerns or alternative interpretations in your answers.<br />
PROFESSIONAL pro<strong>to</strong>col ... Engineers do not cheat on <strong>the</strong> job and <strong>the</strong>y certainly don’t cheat on exams.<br />
Do not open until “START” is announced.
E 45 Midterm 02 SOLUTIONS:<br />
1. Defects in Solids (10 points)<br />
Mark ☒ <strong>the</strong> ballot box corresponding <strong>to</strong> <strong>the</strong> best answer.<br />
Two (+2) points for correct answers, -1 if wrong, 0 if blank.<br />
(a) Point defects in solids include<br />
☒ vacancies<br />
☐ dislocations<br />
☐ both<br />
(b) The defect known as a “Frenkel pair” is shown in this<br />
sketch <strong>to</strong> have<br />
☐ body-centered symmetry<br />
☒ an extended strain field<br />
☐ both<br />
(c) Vacancies in solids<br />
☐ participate in diffusion<br />
☐ increase <strong>the</strong> entropy of a material<br />
☒ both<br />
(d) Dislocations in solids<br />
☒ participate in plastic deformation<br />
☐ decrease <strong>the</strong> entropy of a material<br />
☐ both<br />
(e) Fick’s First Law for diffusion flux<br />
Jx = −D ∂c<br />
∂x<br />
expresses <strong>the</strong> fact that<br />
☐ diffusion requires a negative diffusivity<br />
☒ mass flows down a concentration gradient<br />
☐ both<br />
page 2 of 6<br />
2. Defects in Solids (10 points)<br />
For this problem you must <strong>draw</strong> and label all requested<br />
features directly on <strong>the</strong> figures provided.<br />
(a) (2 points) Fill in <strong>the</strong> a<strong>to</strong>ms comprising <strong>the</strong> extra-half<br />
plane and label with <strong>the</strong> conventional symbol (⊥) <strong>the</strong> edge<br />
of <strong>the</strong> extra half-plane that establishes <strong>the</strong> line direction<br />
vec<strong>to</strong>r of <strong>the</strong> edge dislocation shown <strong>below</strong>.<br />
(b) (3 points) On <strong>the</strong> same figure <strong>below</strong>, trace and label a<br />
Burgers circuit in finish-start-right-hand (FSRH) convention,<br />
and identify <strong>the</strong> resulting Burgers vec<strong>to</strong>r (b).<br />
b 1<br />
F<br />
3<br />
S<br />
2<br />
1<br />
3<br />
(c) (2 points) Fill in <strong>the</strong> a<strong>to</strong>ms comprising <strong>the</strong> extra-half<br />
plane and label with <strong>the</strong> conventional symbol (⊥) <strong>the</strong> edge<br />
of <strong>the</strong> extra half-plane that establishes <strong>the</strong> line direction<br />
vec<strong>to</strong>r of <strong>the</strong> edge dislocation shown <strong>below</strong>.<br />
(d) (3 points) On <strong>the</strong> same figure, <strong>draw</strong> in and label <strong>the</strong><br />
location of <strong>the</strong> slip plane on which this edge dislocation<br />
glides.<br />
2<br />
2<br />
Slip<br />
Plane<br />
3<br />
1<br />
1<br />
3<br />
2
E 45 Midterm 02 SOLUTIONS:<br />
3. Phases and Phase Equilibria (10 points)<br />
Refer <strong>to</strong> <strong>the</strong> Cu-Zn binary <strong>phase</strong> <strong>diagram</strong> <strong>below</strong> (from ASM<br />
Metals Handbook, 8 th edition, Vol. 8, (1973), p. 301) <strong>to</strong><br />
answer <strong>the</strong> following questions. Recall that “brass” is <strong>the</strong><br />
common name applied <strong>to</strong> this alloy.<br />
T (°C)<br />
1100<br />
1000<br />
900<br />
800<br />
700<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
0<br />
Cu<br />
at % Zn<br />
10 20 30 40 50 60 70 80 90<br />
"<br />
903°<br />
(a)<br />
456°<br />
(b)<br />
!<br />
!’<br />
(c)<br />
468°<br />
10 20 30 40 50 60 70 80 90<br />
wt % Zn<br />
#<br />
L<br />
835°<br />
(d)<br />
700°<br />
598°<br />
$<br />
558°<br />
424°<br />
% &<br />
(a) (2 points) What is <strong>the</strong> maximum concentration of Zn<br />
that can be dissolved in α brass?<br />
Ans: 39 wt. % Zn<br />
(b) (2 points) Apply <strong>the</strong> <strong>phase</strong> rule (F = C-P+1) <strong>to</strong> calculate<br />
<strong>the</strong> number of degrees of freedom available <strong>to</strong> a 40<br />
wt% Zn alloy at room temperature.<br />
Ans: F = 2 - 2 + 1 = 1<br />
(c) (2 points) What <strong>phase</strong>(s) is (are) in equilibrium when<br />
β brass (50:50 composition) is held at 500°C.<br />
Ans: β + γ<br />
(d) (2 points) Write <strong>the</strong> reaction that occurs on cooling<br />
through <strong>the</strong> 700°C peritectic iso<strong>the</strong>rm.<br />
Ans: γ + L ➔ δ<br />
(e) (2 points) Both <strong>the</strong> ε and η <strong>phase</strong>s of brass have hexagonal<br />
crystal structures. What composition would yield<br />
equal weight fractions of <strong>the</strong> <strong>the</strong>se two <strong>phase</strong>s in equilibrium<br />
at 100°C?<br />
Ans: 92.5 wt % Zn<br />
(e)<br />
Zn<br />
page 3 of 6<br />
4. Phases and Phase Equilibria (10 points)<br />
These questions refer <strong>to</strong> <strong>the</strong> same Cu-Zn binary <strong>phase</strong> <strong>diagram</strong><br />
from Problem 3.<br />
(a) (5 points) Sketch <strong>the</strong> microstructure resulting when a<br />
70 wt% Zn alloy with initially large γ grains at 550°C, as<br />
shown <strong>below</strong>, is cooled slowly <strong>to</strong> room temperature. Label<br />
all <strong>phase</strong>s.<br />
Slow cooling will result in grain<br />
boundary precipitation of <strong>the</strong> ε <strong>phase</strong><br />
(volume fraction ≈ 25%) within <strong>the</strong> γ<br />
grains (volume fraction ≈ 75%)..<br />
(b) (5 points) The eutec<strong>to</strong>id composition at 558°C is 74.1<br />
wt % Zn. Sketch <strong>the</strong> microstructure resulting when an alloy<br />
of this composition, showing a δ <strong>phase</strong> morphology at<br />
560°C as shown <strong>below</strong>, is cooled slowly <strong>to</strong> room temperature.<br />
Label all <strong>phase</strong>s.<br />
!<br />
"<br />
! "<br />
At <strong>the</strong> eutec<strong>to</strong>id iso<strong>the</strong>rm, all of <strong>the</strong> δ<br />
<strong>phase</strong> will decompose <strong>to</strong> <strong>the</strong> ε + γ in a<br />
lamellar constituent, in volume fractions<br />
of 40% ε and 60% γ.
E 45 Midterm 02 SOLUTIONS:<br />
7. Metallic <strong>Al</strong>loys (10 points)<br />
Temper Definition<br />
H1 Strain-hardened<br />
H2 Strain-hardened, partially annealed<br />
T3 Solution-treated, cold-worked, naturally<br />
aged<br />
T6 Solution-treated, artificially aged<br />
T9 Solution-treated, artificially-aged, cold<br />
worked<br />
The above table is a partial list of <strong>the</strong> “temper designations”<br />
for aluminum alloys specified by <strong>the</strong> <strong>Al</strong>uminum Association<br />
and published in <strong>the</strong> ASM Metals Handbook, 9 th<br />
edition, Volume 2 (1979). Recognizing that <strong>the</strong> specified<br />
treatments appearing in <strong>the</strong> “definition” column occur in<br />
sequence, and in <strong>the</strong> order given, rank <strong>the</strong> various temper<br />
treatments in order of highest strength <strong>to</strong> lowest strength.<br />
1. T9<br />
2. T3<br />
3. T6<br />
4. H1<br />
5. H2<br />
Reasoning: In general, <strong>the</strong> combination of work-hardening<br />
and precipitation hardening gives <strong>the</strong> highest overall<br />
strength. The T3 temper designation is <strong>the</strong> one given <strong>to</strong><br />
aircraft rivets, as described in lecture. Strain hardening<br />
alone can be considerable, but if an alloy was designed <strong>to</strong><br />
be precipitation-hardened (by choice of suitable alloying<br />
additions in appropriate amounts), it is expected that an<br />
aging treatment can also be designed <strong>to</strong> maximize strength<br />
without <strong>the</strong> damage of cold work. Those alloys for which<br />
<strong>the</strong> only available streng<strong>the</strong>ning option is strain hardening<br />
would be treated <strong>to</strong> earn an H designation, with a judicious<br />
amount of cold-work <strong>to</strong> avoid non-uniform stress distributions<br />
that might lead <strong>to</strong> cracking and/or brittle fracture.<br />
Annealing of course softens a material, putting it at <strong>the</strong><br />
bot<strong>to</strong>m of <strong>the</strong> list.<br />
page 5 of 6<br />
8. Metallic <strong>Al</strong>loys (10 points)<br />
Streng<strong>the</strong>ned by Weakened by<br />
Porosity (casting)<br />
Cold working Annealing<br />
<strong>Al</strong>loying Welding<br />
Phase Transformations Phase Transformations<br />
The above table lists some of <strong>the</strong> general effects of “processing”<br />
of metals and alloys on <strong>the</strong>ir mechanical strength.<br />
For example, an alloy used in <strong>the</strong> “as-cast” condition is<br />
generally weaker due <strong>to</strong> <strong>the</strong> porosity that occurs because of<br />
air entrapment during solidification from <strong>the</strong> liquid <strong>phase</strong>.<br />
Similarly, welding is listed as a cause of “weakening,” due<br />
<strong>to</strong> <strong>the</strong> fact that <strong>the</strong> local application of heat needed <strong>to</strong> weld<br />
alloys causes significant a<strong>to</strong>mic transport, including some<br />
in <strong>the</strong> liquid <strong>phase</strong>.<br />
Explain why “<strong>phase</strong> transformations” is listed in both columns.<br />
Answer: The <strong>phase</strong> transformations in <strong>the</strong> “streng<strong>the</strong>n”<br />
column are those that cause precipitation hardening. Such<br />
transformations result from carefully controlled <strong>the</strong>rmal<br />
treatments, beginning with homogenization in a single<br />
<strong>phase</strong> field, followed by rapid quenching <strong>to</strong> generate a supersaturated<br />
solid solution, finishing with an aging treatment<br />
<strong>to</strong> produce a fine dispersion of second <strong>phase</strong> particles<br />
that impede dislocation motion.<br />
The <strong>phase</strong> transformations in <strong>the</strong> “weaken” column<br />
are those that are not carefully controlled, such as<br />
slow cooling from <strong>the</strong> homogenization temperature, which<br />
usually results in a detrimental distribution of second <strong>phase</strong><br />
particles occurring exclusively at grain boundaries. The<br />
grain interiors are <strong>the</strong>refore made much less resistant <strong>to</strong><br />
dislocation motion because <strong>the</strong>y have no precipitate particles<br />
<strong>to</strong> serve as obstacles, and many fewer solute a<strong>to</strong>ms that<br />
also serve as impediments <strong>to</strong> dislocation motion (stronger<br />
metallic bonding). When such a material is deformed, dislocations<br />
move freely through <strong>the</strong> grains, sometimes with<br />
even lower strength than <strong>the</strong> solution solution would have<br />
shown.
E 45 Midterm 02 SOLUTIONS:<br />
9. Ceramics and Glasses (10 points)<br />
An important family of “magnetic” ceramics is <strong>based</strong> <strong>upon</strong><br />
<strong>the</strong> spinel (Mg<strong>Al</strong>2O4) structure. Spinel is formed from an<br />
fcc Bravais lattice and a basis of fourteen (14) ions per lattice<br />
point: 2 Mg 2+ , 4 <strong>Al</strong> 3+ and 8 O 2- . The magnesium ions<br />
are tetrahedrally coordinated by four oxygen ions, while<br />
<strong>the</strong> aluminum ions are octahedrally coordinated by six<br />
oxygen ions. Note that both <strong>the</strong> motif and <strong>the</strong> chemical<br />
formula preserve charge neutrality.<br />
However, <strong>the</strong> magnetic (known as “ferrimagnetic”) version<br />
of this structure is called an “inverse spinel,” in which <strong>the</strong><br />
octahedral sites are occupied by <strong>the</strong> divalent ions and onehalf<br />
of <strong>the</strong> trivalent ions, while <strong>the</strong> remaining trivalent ions<br />
are in <strong>the</strong> tetrahedral sites.<br />
One example of <strong>the</strong> ferrimagnetic ceramics is magnetite,<br />
<strong>the</strong> naturally occurring “lodes<strong>to</strong>ne” that was used <strong>to</strong> make<br />
<strong>the</strong> original compass. It is also found in meteorites. This<br />
could be <strong>the</strong> reason why, in Fox's hit series The X-Files,<br />
FBI investiga<strong>to</strong>rs observed that magnetite could disrupt<br />
alien life forms, often causing <strong>the</strong>ir death or destruction (?).<br />
Magnetite is an inverse spinel, yet its chemical formula is<br />
Fe3O4. Explain.<br />
Answer: The apparent anomaly here is charge balance. If<br />
you count up <strong>the</strong> number of negative charges on <strong>the</strong> eight<br />
(8) O 2- ions (= -16) and compare that number with <strong>the</strong><br />
number of positive charges on six (6) Fe 2+ ions (= +12),<br />
you arrive at a conundrum. However, taking a clue from<br />
<strong>the</strong> opening paragraph above, a spinel consists of both divalent<br />
and trivalent cations in <strong>the</strong> correct ratio (2 of <strong>the</strong><br />
divalent species and 4 of <strong>the</strong> trivalent species (= +16) <strong>to</strong><br />
achieve charge neutrality. So, if <strong>the</strong> chemical formula of<br />
magnetite is correct, its charge distribution must be reconciled.<br />
And <strong>the</strong> way <strong>to</strong> do that is <strong>to</strong> give Fe a multivalent<br />
character. Assume that it can be ei<strong>the</strong>r divalent or trivalent.<br />
The answer <strong>the</strong>n is that <strong>the</strong>re are must be two (2) Fe 2+ ions<br />
and four (4) Fe 3+ ions in this inverse spinel. You can think<br />
of <strong>the</strong> chemical formula in <strong>the</strong> same format as that for <strong>the</strong><br />
original spinel, Mg<strong>Al</strong>2O4, which would be expressed as<br />
FeFe2O4, but <strong>the</strong> more efficient form is Fe3O4.<br />
page 6 of 6<br />
10. Ceramics and Glasses (10 points)<br />
The following plot shows <strong>the</strong> <strong>the</strong>rmal expansion behavior<br />
typical of a glass. Note that strain is plotted on <strong>the</strong> vertical<br />
axis, with temperature increasing <strong>to</strong> <strong>the</strong> right on <strong>the</strong> horizontal<br />
axis. At <strong>the</strong> softening temperature (Ts), <strong>the</strong> glass is<br />
unable <strong>to</strong> support its own weight and flows freely, invalidating<br />
<strong>the</strong> <strong>the</strong>rmal expansion data.<br />
!L / L 0<br />
During <strong>the</strong> processing of safety glass for windows, a treatment<br />
is used <strong>to</strong> place <strong>the</strong> surface of <strong>the</strong> glass in residual<br />
compression, so that it will not be as susceptible <strong>to</strong> fine<br />
surface cracks. In one of <strong>the</strong>se treatments, <strong>the</strong> glass is first<br />
equilibrated above its glass transition temperature (Tg).<br />
Next it is subjected <strong>to</strong> cold air blast on both sides, a “surface<br />
quench,” <strong>to</strong> form a rigid but thin “skin” on both surfaces.<br />
The skin is cool enough <strong>to</strong> remain <strong>below</strong> <strong>the</strong> glass<br />
transition temperature while <strong>the</strong> interior of <strong>the</strong> glass is still<br />
above Tg. The glass is <strong>the</strong>n allowed <strong>to</strong> cool slowly and<br />
uniformly <strong>to</strong> room temperature.<br />
Explain how this treatment causes residual surface compression.<br />
Answer: The schematic at<br />
right shows how <strong>the</strong> stress<br />
distribution varies with each<br />
<strong>the</strong>rmal treatment. The residual<br />
surface compression<br />
comes during <strong>the</strong> final stages<br />
of cooling, when <strong>the</strong> larger<br />
interior mass of glass contracts,<br />
pulling <strong>the</strong> surface skin<br />
in<strong>to</strong> compression.<br />
T g<br />
T 0<br />
T g<br />
T 0<br />
T g<br />
T 0<br />
T g<br />
T f<br />
Temp<br />
T s<br />
T<br />
Compression<br />
0<br />
Tension<br />
Compression<br />
0<br />
Tension<br />
Compression<br />
0<br />
Tension<br />
Stress