Lecture 8 Flashcards

1
Q

if crack in material

A

stress concentration around crack is very high - very large a tip of crack

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2
Q

size and shape of crack determine

A

stress concentration and whether a material can support it or not

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3
Q

stress intensity factor Ki Pam^0.5 linked to

A

can be linked to the toughness of a material

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4
Q

stress intensity factor equation

A
geometry factor (dimensionless) * applied stress * sqrt(pi * crack size)
Ki= Y* sigma * sqrt(pi *a)
i determines the type of crack propagation mode
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5
Q

K1

A

mode 1 tensile fracture crack plane normal to direction of the largest tensile loading
mode 2 would be shear
mode 3 tearing
only look at mode 1

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6
Q

K1c and typical values

A

is the critical stress intensity factor above which the material can not support brittle failure
aluminium alloy 36 MPam^0.5
steel 50MPam^0.5 can support cracks up to a larger load
low value means cannot support crack

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7
Q

centre crack

A

length of crack is 2a therefore need to divide length by 2 to get a

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8
Q

in an infinite plate centre crack Y is

A

1 crack length equal to twice a

l = 2a

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9
Q

in an infinite plate edge crack Y is

A

1.12 crack length equal to a

l = a

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10
Q

what does an infinite plate

A

a/width of plate, if value is very small much more like a infinite plate (width here is dimension parallel to crack) material around crack is well supported if a/w approaches 1 then material around crack not very well supported

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11
Q

For a finite plate equation

A

can be found on formula sheet equation for both edge and centre crack this equation tends to 1 for a centre crack a/w is very small and to 1.12 for a edge crack where a/w is very small

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12
Q

if calculated value of K1 is lower than K1c and if higher

A

material can support crack
if higher can not support crack material fails catastrophically brittle manner
larger crack material more likely to fail

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13
Q

materials can fail below their normal strength due to

A

temperature
cracks and stress concentration
fatigue
creep

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14
Q

fatigue is

A

low amplitude vibrations below the yield point of the material causes dislocation of defects to move to a similar region and therefore material fails in brittle manner

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15
Q

fatigue is particularly important for

A

aircraft as goes through many cycles

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16
Q

as we apply a oscillatory stress to it

A

its strength begins to fall over many cycles

17
Q

endurance limit taken at

A

10^7 cycles (10^7 oscillations) we find where material crosses this

18
Q

steels show fatigue limit of

A

40% of yield strength

19
Q

ferrous metals fatigue limit

A

drop in yield strength flattens off and end with fatigue limit below which the yield strength does not drop any further no matter how many cycles

20
Q

non ferrous metal do not

A

hit fatigue limit will just continue to decrease until material breaks - very important to suit material to your application and life span of

21
Q

creep is

A

a thermal effect - materials placed under stresses at elevated temperatures way below melting point but enough energy to cause vibrations
slowly deforms over time
load changes bonding potential and temperature helps atoms slowly move out

22
Q

creep defined as

A

time dependent and permanent deformation of materials when subjected to constant load or stress

23
Q

which is worse edge crack or centre crack of same length under same load and why

A

look at stress intensity factor equation
for edge crack a is larger as centre crack a=l/2
for edge crack geometrical factor is larger 1.12 > 1
therefore requires lower stress to achieve same stress intensity factor - material fails at lower stress