hey everyone I wanted to talk about heat
treating steel a
little bit in this
video so if you
search for this topic on
the internet you'll
find there's a lot
of theoretical and
background
information and then
also a lot of
practical
information without much
explanation of why
the things are done
so I'm hoping to
bridge the gap a little
bit in this video
when we talk about
heat treating steel
we're mostly
interested in
increasing the materials
strength by exposing
it to different
temperatures in sort
of a prescribed way
but first a note
about what strength
actually is there's
a few different
quantities to keep
in mind here the main
ones being stiffness
and strength so
here's a graph here
and it says strain
on the bottom and
stress on the vertical
axis and what we're
showing here is how
hard we're pulling
on the material here
the stress is the
force divided by the
area and the strain
is how far the
material is moved so
this is the the
Delta how much the
material has actually
elongated or
contracted divided by its
total length so this
graph takes into
account whatever
size material you might
have so for steels
and most ductile
materials when we
start yanking on the
material that will
deform a little bit
and if we don't yank
too hard we can let
go and the material
wills elastically
returned back to its
original shape so
if we take this
steel bar here and I
flex it a little bit
it snaps back to
its straight shape
with no problem and
so what's happening
here on the graph as
I'm taking it up to
about this point and
letting it back down
instead if I take
this coat hanger and
stretch it a little
bit now when I let
go the curve actually
stays in the coat
hanger so on the graph
what's happened is
I've stressed it so
the stress has gone
up and eventually
we've gone so far
that it's gone past
its yield point and
now we're in a
region called the
plastic region so we
put a plastic
deformation in this coat
hanger by bending it
like this what's
important to note is
that we can have a
very stiff material
that's not very
strong or we could
have a very
material that's not
very stiff the two
quantities are
actually not dependent on
each other so let's
pretend this line
represented steel
aluminum on this graph
might look something
more like this and
there's a lot to
talk about with this
graph but I'm just
going to do sort of a
general kind of
overview but
hypothetically let's
say we had an
aluminum alloy that
looked like this its
strength could
actually be equal to the
steel now it's not
going to be as stiff
because the
stiffness is actually a
material property
and we can't easily
change the stiffness
through heat
treatment we would
probably have to use
a different material
if we needed a
different stiffness
but if we had this
this great aluminum
alloy we could say
well it's just as
strong as steel
because the
stress-strain point where
the material gives
out and doesn't
spring back anymore
is actually at the
same stress however
the material has
moved more in that
in that loading
because it's not as
stiff the x over
here indicates the
point of breakage and
so if we keep
pulling this material
farther and farther
eventually we're
into this plastic
region where we can
change the shape of
the material without
putting in all that
much additional
stress and then
eventually the material
gives out and it
breaks so when we heat
treat steel we're
actually staying on
this same slope here
because we can't
change the stiffness
of it but what we
can do is move the
yield point up
through heat
treatment so let's just say
we had a material
that looked like this
now this material is
just as stiff as
the original one
it's still steel but it
has a much higher
yield point so we say
that it's stronger
one of the downsides
though is that this
line doesn't go over
into the plastic
region as far so what
happens with this
material is we load it
and it's still
elastic it's still
elastic and then
there's a tiny amount
of plastic
deformation but it breaks
right away this is
characteristic of
extremely hard
steels and it's also
characteristic of
brutal materials
like glass so if we
took a piece of
glass just like a window
and flexed it we
could let go and it
would snap back to
its you know flat
shape but eventually
if we flexed it too
far it would just
break all of a sudden
without really much
warning and we can't
take a piece of
glass and bend it and
then let go and
expect it to retain that
shape so glass is a
brittle material
because it doesn't
have this plastic
region you'll also
note that it says
maximum tensile
strength here instead of
here so what's the
deal with that like
why why do we
actually count this as the
material strength
the reason is that
let's say we were
building like an
airplane part or
something that you
wanted to support a
load in an important
way if the material
is in this plastic
region the part has
deformed enough
where it might be
causing problems so
let's say this or an
airplane landing
gear if you're up in
this region over
here the landing
gear is not going to be
the same shape
anymore so it's true that
you might get a
little bit of additional
strength out of the
material but you
really can't count
on that part being
sound anymore so for
engineering this is
the point where we
say the material has
failed it's yielded
so the weight a
hardened steel is to
heat it up until
it's glowing red and
then very quickly
reduce the
temperature by plunging it in
water or oil
typically and what happens
this is the
crystalline structure inside
the steel changes so
it's very different
from letting the
steel cool down slowly
and that rapid
cooling is actually what
causes us to make
the graph that looks
like this instead of
like this but we
have a problem
I just said that
this is behavior is
like glass where you
load the material
and then suddenly it
breaks really
without much warning
and we don't really
like that behavior
in very many
materials and
another problem is that
the really freshly
hardened steel like
if you heat the
steel up dump it in
water take it out
it's so incredibly
hard and brittle
that you can break it
very easily even
with your hands at the
steel if the piece
is small enough so
typically all
hardening operations are
followed by a
tempering operation and
the tempering
operation actually
lowers the strength
of the material but
it increases the
toughness so there's a
very distinct
trade-off there and the
tempering process
can be tailored to
give us any sort of
a a strength versus
toughness trade-off
so for example let's
say we tempered it
so that we had a
material that looked
like this instead
of going all the way
to full hardness we
could temper the
material and maybe we'd
end up with
something like that so now
we've got all this
extra room here in
the plastic region
and it's not quite as
strong as the as the
full hard but the
tempered steel is
much much more easy to
use in an
engineering application
because it's not
like glass it's more
like a normal metal
so to test this out
I bought some w1
steel this is an eighth
of an inch in
diameter and w1 means
water hardening so
this steel is meant
to be heated up and
then tossed in water
to quench it to cool
it down and harden
it and then you can
temper it to give
you any sort of a
curve a desired
toughness and
strength and to test it I
came up with this
little test jig here
so that I could load
the samples in
bending and
carefully apply more load by
hanging a bucket
from it and I filled
the bucket up with
sand and bits of
metal to see how
much load I could hold
with each with each
piece of steel with
each sample and what
I did as I started
off these samples
are untreated so this
is probably not
fully annealed when I
talked about cooling
the steel down and
you have a couple
options you could heat
it up to red-hot and
then cool it down
really really slowly
by like putting it
in an oven or in an
insulator and that
will give you full
anneal that's the
softest you can get
if you heat the
steel up and just
let it cool down in
air that's called
normalized and so even
that will give you
some amount of
hardening over the
full and yield state
and I don't know how
this is sold for
mcmaster this is
probably normalized so
they heated this up
and then let it cool
down at ambient
temperature I'm guessing
but it's it's
relatively soft and so I
was able to bend it
by
this just by
applying 16 kilograms so
note that we
actually didn't get to
breakage on this
piece what would happen
to us since we went
up the graph and
then stopped
somewhere around here so it
was plastic and
eventually just slipped
out at the fixture
if we kept bending it
eventually we get to
fracture and it
would break so next
I tested one of
these full hard
pieces and this one I
heated up to you
know cherry red and
then dropped it in
water and took it out
and put it in the
loading jig and this
one only held six
kilograms and also as
you can see there's
no bending at the
fracture so that we
have this sort of a
situation where it
elastically deformed
you can see it
bending a little bit when
we load it and then
suddenly it
fractures and snaps
back there's very
little if any
plastic deformation at the
breakage point now
you might be saying
well this only held
six kilograms and
the soft one held
you know sixteen point
two kilograms you
know what's the deal
with that I thought
we were supposed to
be getting a lot
more out of this and
the answer is that
point loading is a
very complex thing
and so if we have a
bar like this with a
steel cable loading
it like this right
at the point where
the steel cable is
touching it there
could be an
additional stress caused by
this loading scheme
this is also the
reason that glass is
not considered a
structural material
because you can't
really clamp a piece
of glass without
introducing a lot of
local stresses that
would break it so
you can really think
of super hard steel
like this as a piece
of glass where it's
very um it's very
touchy and so small
small amounts of of
local stress will
cause it to fat to
fracture which is
why it's basically
never used so now
we've covered the
extreme ends of this
spectrum we've gone
from normalized or
very soft to full
hard which is almost
unusable because
it's just so brittle
so to temper the
steel what we do is
we heat it up a
little bit and then
let it cool down
slowly and what
happens here is we give
up some of this
hardness because we're
letting
that crystalline
structure changed by
heating it up a
little bit and if we
heat it up to a very
specific
temperature we can
control how much
strength were
actually trading for
toughness very
conveniently steel will
change color in air
based on how how
high we heat it up
and the color change
comes from an oxide
layer that's forming
on the steel and
it's interfering with
light and we can see
what color or what
temperature the
steel is based on what
color we see off
that because the oxide
layer is forming an
optical interference
pattern there so as
we heat it up we'll
see a straw yellow
color and then kind
of an orange color
and then brown and
purple and then blue
and then light blue
and the hotter we
heated up the more
strength we give up
in return for
getting more
toughness and so there's
quite a bit of
research and fine-tuning
to be done here but
for home shop
hardening and
tempering it's actually
quite ineffective
and decent means of
setting up tooling
of course if you have
access to a kiln it
also makes a lot
more sense to just
set the temperature
that you want to
temper your steel to
and put it in the
kiln and leave it for
the prescribed time
which is actually
like an hour -
usually and then take it
out of the kiln and
let it cool down so
interestingly enough
I started with the
the 300 degree
Celsius piece that I kiln
tempered and this
piece held about 55
kilograms in fact my
bucket became
overloaded I put all
of the sand in
there and that it
was holding fine and
then I put all kinds
of random scrap
bits of metal in
there and it was still
holding and I had to
push down on it
with my arms so I I
completely didn't
expect how strong I
could actually make
this steel compared
to the full hard and
the normalized state
the results for the
other tempered pieces
were pretty
similar except for
this one this one i
tempered only two
straw yellow which is
less tempering which
means more brittle
and stronger so I
stopped recording how
much weight these
things held because my
system was woefully
in
but what was interesting
is that this
one broke in a
brittle sort of a
fracture whereas
these other tempered
pieces that were
tempered to higher
temperatures did not
break like that
these yielded
another really handy trick
is to use the file
to determine how hard
the material is that
we're working with
so these normalized
pieces if you just
lightly run a file
along and I'm hardly
pressing down on the
file I'm just
pushing it along
very gently you can see
that it sort of
grabs and after you do
this a few times so
we get a very good
feel for what
different steals at behave
like but this is
very grabby and if we
take one of the full
hard pieces the the
file just absolutely
glides along like
it's on glass it's
not even biting into
the material at all
and that's because
this is actually
harder than the file so
when we drag the
file teeth across there
and the teeth don't
dig into the metal
at all whereas with
a softer one the
file teeth actually
bite in and that's
what's causing the
drag also I should
point out that
hardness is related to
strength so when we
say a material is
really hard what we
mean is it's
actually very strong
and files are quite
hard it's actually
one of the hardest
tools that you'll
find in a common
machine shop and the
fact that we can
run it across this
and this is actually
even harder than the
file seemed would
indicate that this
is something that
this is a hardness
that you generally
not encounter here's
a graph that shows
what's actually
happening when we cool
down a piece of
steel so this is the
first part of the
process the hardening
part of the process
and we've got
temperature on the
y-axis and time and
the x-axis and we're
starting off at
about 800 degrees C
which is the cherry
red color and what
we want to do is get
down into this phase
down here we want
to get below this
line without going
through this part of
the graph so this
whole deal with
cooling it down quickly
is because we need
to get down to this
part of the graph
without interfering
with this area this
graph is called the
time temperature
transformation graph
and we talked about
going past the
those of the TTT
graph like this and so
there's this
critical cooling rate where
we have to get down
into here around so
we don't get this
hardening effect so if
we take too long if
we if we spend ten
seconds cooling down
from 800 we're
gonna end up in this
region and that
means that we'll get
some hardness so
there'll be some
hardening effect but it
won't be anywhere
near getting down to
here and if you're
curious the M is
martensite which is
the crystalline
structure that gives
us that really high
hardness in steel
when we temper the
steel we're actually
starting out down
here and we take it
up into this region
so we're basically
giving up some of
this really hard
crystalline structure
and gaining some of this
less hard but
tougher structure
and there's a lot of
terminology involved
here that probably
won't help you
understand it but if you
go searching for
this stuff you'll find
quite a depth of
information so you
might be wondering
what can I do this
trick with a coat
hanger if I heat it up
and then cool it
down and do this sort
of transformation no
the answer is nope
you need to have
steel that is hardened
abaut and not all
steels are hardened
Abul and the thing
that determines
whether they're
hardened Abul or not is
the carbon content
and to a lesser
extent the other
alloying ingredients so
this w 1 water
hardening steel that I've
been using today has
a carbon content
fairly close to 1 1
% so this graph
shows us temperature
on the y axis and
carbon content as a
percent on the x
axis and most tool
steels are pretty
close to about 1%
and the reason for
that is that it
makes this crystalline
structure that's
very beneficial for
having a very hard
structure if we have
tons and tons of
carbon what we actually
have is cast iron
and if we have very
little carbon we
have cheap steel
basically ok well I
hope that was
helpful
see you next time
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