Lecture 8 Flashcards
if crack in material
stress concentration around crack is very high - very large a tip of crack
size and shape of crack determine
stress concentration and whether a material can support it or not
stress intensity factor Ki Pam^0.5 linked to
can be linked to the toughness of a material
stress intensity factor equation
geometry factor (dimensionless) * applied stress * sqrt(pi * crack size) Ki= Y* sigma * sqrt(pi *a) i determines the type of crack propagation mode
K1
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
K1c and typical values
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
centre crack
length of crack is 2a therefore need to divide length by 2 to get a
in an infinite plate centre crack Y is
1 crack length equal to twice a
l = 2a
in an infinite plate edge crack Y is
1.12 crack length equal to a
l = a
what does an infinite plate
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
For a finite plate equation
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
if calculated value of K1 is lower than K1c and if higher
material can support crack
if higher can not support crack material fails catastrophically brittle manner
larger crack material more likely to fail
materials can fail below their normal strength due to
temperature
cracks and stress concentration
fatigue
creep
fatigue is
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
fatigue is particularly important for
aircraft as goes through many cycles
as we apply a oscillatory stress to it
its strength begins to fall over many cycles
endurance limit taken at
10^7 cycles (10^7 oscillations) we find where material crosses this
steels show fatigue limit of
40% of yield strength
ferrous metals fatigue limit
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
non ferrous metal do not
hit fatigue limit will just continue to decrease until material breaks - very important to suit material to your application and life span of
creep is
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
creep defined as
time dependent and permanent deformation of materials when subjected to constant load or stress
which is worse edge crack or centre crack of same length under same load and why
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