|
Annealing
The purpose
of annealing may involve one or more of the following aims:
To soften
the steel and to improve machinability.
To relieve internal stresses induced by some previous treatment
(rolling, forging, uneven cooling).
To remove coarseness of grain.
The treatment is applied to forgings, cold-worked sheets and
wire, and castings. The operation consists of:
heating
the steel to a certain temperature,
"soaking" at this temperature for a time sufficient
to allow the necessary changes to occur,
cooling at a predetermined rate.
Sub-critical Anneal
It is not always necessary to heat the steel into the critical
range. Mild steel products which have to be repeatedly cold
worked in the processes of manufacture are softened by annealing
at 500° to 650°C for several hours. This is known
as "process" or "close" annealing, and
is commonly employed for wire and sheets. The recrystallisation
temperature of pure iron is in the region of 500°C consequently
the higher temperature of 650°C brings about rapid recrystallisation
of the distorted ferrite Since mild steel contains only a
small volume of strained pearlite a high degree of softening
is induced. As shown, Fig. 1b illustrates the structure formed
consisting of the polyhedral ferrite with elongated pearlite
(see also Fig. 2).
Prolonged
annealing induces greater ductility at the expense of strength,
owing to the tendency of the cementite in the strained pearlite
to "ball-up" or spheroidise, as illustrated in Fig.
1c. This is known as "divorced pearlite". The ferrite
grains also become larger, particularly if the metal has been
cold worked a critical amount. A serious embrittlement sometimes
arises after prolonged treatment owing to the formation of
cementitic films at the ferrite boundaries. With severe forming
operations, cracks are liable to start at these cementite
membranes.

Figure
1. Effect of annealing cold-worked mild steel

Figure
2. Effect of annealing at 650°C on worked steel. Ferrite
recrystallised. Pearlite remains elongated (x600)
The modern
tendency is to use batch or continuous annealing furnaces
with an inert purging gas. Batch annealing usually consists
of 24-30 hrs 670°C, soak 12 hrs, slow cool 4-5 days. Open
coil annealing consists in recoiling loosely with controlled
space between wraps and it reduces stickers and discoloration.
Continuous annealing is used for thin strip (85% Red) running
at about 400 m/min. The cycle is approximately up to 660°C
20 sec, soak and cool 30-40 sec. There is little chance for
grain growth and it produces harder and stiffer strip; useful
for cans and panelling.
"Double
reduced" steel is formed by heavy reduction (~50%) after
annealing but it suffers from directionality. This can be
eliminated by heating between 700-920°C and rapidly quenching.
Full
Anneal and Normalising Treatments
For steels with less than 0,9% carbon both treatments consist
in heating to about 25-50°C above the upper critical point
indicated by the Fe-Fe3C equilibrium diagram (Fig. 3). For
higher carbon steels the temperature is 50°C above the
lower critical point.

Figure
3. Heat-treatment ranges of steels
Average
annealing and hardening temperatures are:
|
Carbon,
%
|
0.1
|
0.2
|
0.3
|
0.5
|
0.7
|
0.9
to 1.3
|
|
Avg.temp.
°C
|
910
|
860
|
830
|
810
|
770
|
760
|
These
temperatures allow for the effects of slight variations in
the impurities present and also the thermal lag associated
with the critical changes. After soaking at the temperature
for a time dependent on the thickness of the article, the
steel is very slowly cooled. This treatment is known as full
annealing, and is used for removing strains from forgings
and castings, improving machinability and also when softening
and refinement of structure are both required.
Normalising
differs from the full annealing in that the metal is allowed
to cool in still air. The structure and properties produced,
however, varying with the thickness of metal treated. The
tensile strength, yield point, reduction of area and impact
value are higher than the figures obtained by annealing.
Changes
on Annealing
Consider the heating of a 0,3% carbon steel. At the lower
critical point (Ac1) each "grain" of pearlite changes
to several minute austenite crystals and as the temperature
is raised the excess ferrite is dissolved, finally disappearing
at the upper critical point (Ac3), still with the production
of fine austenite crystals. Time is necessary for the carbon
to become uniformly distributed in this austenite. The properties
obtained subsequently depend on the coarseness of the pearlite
and ferrite and their relative distribution. These depend
on:
a)
the size of the austenite grains; the smaller their size the
better the distribution of the ferrite and pearlite.
b) the rate of cooling through the critical range, which affects
both the ferrite and the pearlite.
As
the temperature is raised above Ac3 the crystals increase
in size. On a certain temperature the growth, which is rapid
at first, diminishes. Treatment just above the upper critical
point should be aimed at, since the austenite crystals are
then small.
By
cooling slowly through the critical range, ferrite commences
to deposit on a few nuclei at the austenite boundaries. Large
rounded ferrite crystals are formed, evenly distributed among
the relatively coarse pearlite. With a higher rate of cooling,
many ferrite crystals are formed at the austenite boundaries
and a network structure of small ferrite crystals is produced
with fine pearlite in the centre.
Overheated,
Burnt and Underannealed Structures
When the steel is heated well above the upper critical temperature
large austenite crystals form. Slow cooling gives rise to
the Widmanstätten type of structure, with its characteristic
lack of both ductility and resistance to shock. This is known
as an overheated structure, and it can be refined by reheating
the steel to just above the upper critical point. Surface
decarburisation usually occurs during the overheating.
During
the Second World War, aircraft engine makers were troubled
with overheating (above 1250°C) in drop-stampings made
from alloy steels. In the hardened and tempered condition
the fractured surface shows dull facets. The minimum overheating
temperature depends on the "purity" of the steel
and is substantially lower in general for electric steel than
for open-hearth steel. The overheated structure in these alloy
steels occurs when they are cooled at an intermediate rate
from the high temperature. At faster or slower rates the overheated
structure may be eliminated. This, together with the fact
that the overheating temperature is significantly raised in
the presence of high contents of MnS and inclusions, suggests
that this overheating is conected in some way with a diffusion
and precipitation process, involving MnS. This type of overheating
can occur in an atmosphere free from oxygen, thus emphasising
the difference between overheating and burning.
As
the steel approaches the solidus temperature, incipient fusion
and oxidation take place at the grain boundaries. Such a steel
is said to be burnt and it is characterised by the presence
of brittle iron oxide films, which render the steel unfit
for service, except as scrap for remelting.
Back
to top
Hardening
and Tempering of Tool Steels
In this
text, an example is tool steel W1, designated only by the
type letter and numeral as used in the USA and the UK for
standardized tool steels. This designation system is so well
known by steel consumers all over the world that no qualifying
institutional designations are necessary.
Carbon
steels and vanadium-alloyed steels
The hardening of these steels, which are made with carbon
contents between 0,80% and 1,20%, is quite straightforward:
Since the rate of carbide dissolution proceeds rapidly, the
holding time, as a consequence, is short and therefore the
heating of small tools can often take place without any extra
precautions against atmospheric oxidation.
The hardening
temperature is about 780°C. Quenching is carried out direct
into brine with tempering following immediately. The quenching
operation is the most critical part of the heat treatment
since too slow a rate of cooling might give rise to either
soft spots or quenching cracks.
If the
tool is designed to contain hardened areas around holes or
reentrant angles the cooling effect must be very intensive
at these areas. Manual stirring will often suffice but in
many cases the coolant must be sprayed on to the tool. For
sections heavier than 20 mm the depth of hardening, i.e. the
distance from the surface to the 550 HV level, is about 4
mm. Sections less than about 8 mm in thickness will harden
through.
For awkward
tools, hardenability may be a crucial factor and under such
circumstances the composition of the steel must be adjusted
in accordance herewith, in particular as regards the alloying
elements Mn and Cr, which have a powerful influence on hardenability.
The diagram
in Figure 1 shows how the hardening temperature affects the
depth of hardening and fracture number on Wl-type steel of
conventional composition. The V-content is only 0,04%, which
implies that the steel starts to be coarse-grained when the
hardening temperature exceeds 815°C.

Figure 1. Depth of hardening for carbon steel, 25 mm in diameter,
corresponding to W1. Quenched in water from various temperatures
In Figure
2 are shown the results of corresponding trials with steel
containing somewhat larger amounts of alloying elements. The
depth of hardening is considerably greater. Owing to the high
content of V the steel remains fine-grained even when hardened
from exceptionally high temperatures.
The very
considerable toughness inherent in plain-carbon steel, due
to its shallow-hardening properties, is forfeited if the tool
through-hardens locally at some sections because the cross-sectional
area there is too small. For shearing tools or small tools
generally, such as scissors, knives or letter die punches,
which are not subjected to heavy impact blows, this drawback
is of less importance. Tools operating under heavy blows,
e.g. upsetting dies for cold-heading of bolts, must not be
through-hardened.
Coining
and striking punches are other examples of carbon tool steels
that require high wear resistance. Such tools may also be
subjected to bending stresses and should therefore not be
through-hardened. The tempering temperature normally used
for tools belonging to this group lies in the range 170°C,
the hardness being generally about 60-64 HRC.

Figure
2. Depth of hardening for carbon steel, 25 mm in diameter,
corresponding to W1. Quenched in water from various temperatures
Back
to top
Heat
Treatment of Low-Alloy Cold-Work Tool Steels
Two
steels have been chosen from this group as examples for the
discussion, grade O1 (RT 1733) and Swedish SIS 2092 (SR 1855).
When
carbon steel is used for punching dies or cold hobbing tools
the dimensions of the tool are bound by a ruling section that
is determined by the load on the tool. A punch or a die, made
from carbon steel, having a diameter of, say, 50 mm, will
show rather poor resistance to sinking on account of the shallow
depth of hardening.
Should
this resistance not suffice, another steel will have to be
chosen, in this case grade O1 or SIS 2092. From the point
of view of heat treatment, these two steels differ somewhat
since their hardening temperatures are different. Steel SIS
2092 requires 850-890°C whereas grade O1 requires 800-840°C.
Owing to its lower hardening temperature, O1 has somewhat
greater dimensional stability. This property makes it a first
choice for blanking dies and other tools requiring a high
degree of dimensional stability (Figure 1).

Figure 1. Blanking tool made from steel O1
In both steels the depth of hardening decreases by roughly
the same amount as the thickness of the section increases.
In the diagram in Figure 2 the hardening temperature was raised
as the cross-sectional area increased in order to increase
the hardenability of the steel. Tools having diameters greater
than about 80 mm or equivalent sections in flat dimensions
are difficult to harden to full hardness if there are re-entrant
corners. For such designs it is advisable to choose SIS 2092
since it obtains full surface hardness more readily and gives
a more regular depth of hardening in a tool with varying section
thickness.

Figure 2. Curves showing depth of hardening for steel O1.
Specimen 25 mm diameter oil quenched from 800°C. Specimen
50 mm diameter oil quenched from 820°C. Specimen 100 mm
diameter oil quenched from 840°C
This
point is well illustrated in Figure 3 which shows longitudinal
sections through test specimens that have been hardened as
normally prescribed for each grade concerned, i.e. oil quenching
for both, from 820°C for grade O1 and from 870°C for
SIS 2092.

Figure 3. Longitudinal section (etched) through stepped test
specimens made from: a) SIS 2092 and b) AISI O1. The diameters
are 50, 75 and 100 mm
The
above-cited example is to be regarded as a practical assertion
of the possibility of estimating the depth of hardening from
the Jominy diagram. However, it should be emphasized once
again that a `contour-hardened` tool is tougher than a through-hardened
one. Figure 4 shows a section through a `contour-hardened`
Pilger roll.

Figure 4. Transverse section through a Pilger roll made from
SIS 2092. Size 50x120 mm
As
a rule both steels are oil quenched. For heavy sections, e.g.
dimensions greater than 100 mm in diameter, it is best to
use water quenching when dealing with SIS 2092. When the surface
temperature of the steel has fallen to between 400°C and
300°C the water quenching is interrupted by transferring
the tool to an oil bath.
The
tempering temperature for both steels is generally in the
range 170-200°C which gives a hardness of more than 60
HRC. As can be seen from Figure 5, SIS 2092 has a greater
resistance to tempering than grade O1.
On
being tempered in the range 250-350°C the steel suffers
a reduction in its impact strength, which in turn increases
the risk of chipping. For this reason tools that are subjected
to impact stresses should not be tempered in this temperature
range. The higher impact strength manifested after tempering
at 170-200°C is due to the presence of retained austenite,
viz. about 10%.

Figure 5. Tempering curves for steel O1 and SIS 2092
This soft retained austenite can accommodate impact stresses
better than the harder constituents. Retained austenite is
decomposed when it is tempered at about 300°C.
If,
during service, some areas of the tool have to support excessive
pressures, for example the shearing edge of circular slitting
knives (see Figure 6), retained austenite may be transformed
to martensite, with spalling at the edge as a result. Should
this occur, tempering at 300-400°C is recommended. After
such a treatment the hardness of SIS 2092 still remains around
60 HRC.
Since
the wear resistance of SIS 2092 is as much as 25% greater
than that of grade O1, the former is very popular when a wear-resisting
steel is required that can give a better performance than
grade O1. Compared with this steel, SIS 2092 has been shown
to have a considerably longer service life, particularly as
drawing die steel.
Another
interesting application is as cane-slitting tools (see Figure
7). The requirements of this type of tool are both high wear
resistance and toughness in its thin walls. Of all the steels
tested the best results were obtained with SIS 2092. In recent
years SIS 2092 has increasingly been used for so-called Pilger
rolls, which are in part made as rings and in part as dies.

Figure 6. Circular shears (slitting knives) made from SIS
2092
Figure
7. Cane-slitting tool made from SIS 2092
Figure 8 shows one of the world`s largest Pilger rolls, designed
for cold-rolling 10 inches tubes. The only steel suitable
for this tool was SIS 2092. Another field of application is
for what are known as Yoder rolls. A sketch showing the principle
of operation and tube manufacture is shown in Figure 9. For
this mill unit, the wear resistance of rolls made from SIS
2092 has shown itself to be on a par with that of grade D2,
in fact in some instances it has outlasted this grade.

Figure 8. Pilger roll made from SIS 2092 for 10 in tube mill.
Dimensions: 800 mm diameter x 400 mm,
weight 800 kg

Figure 9. Sketch showing tube-mill operating principle for
welded tubes (Yoder mill). Welding stage omitted
This
observation is particularly striking when stainless steel
tubes are being rolled, since there is no `galling` when SIS
2092 is being used.
Back
to top
Heat
Treatment of Low-Alloy Cold-Work and Hot-Work Tool Steels
For
considering heat treatment of this group, several typical
tool steels are selected as examples, designated only by the
type letter and numeral as used in the USA and the UK for
standardized tool steels, e.g. H13, O1. These designations
are so well known by steel consumers all over the world that
no qualifying institutional designations are necessary. Steels
for which there are no AISI or BS specifications are designated
according to Swedish (SIS) standards.
The hardenability
of SIS 2550 is considerably good. SIS 2550 is air hardened
in fairly heavy sections, which is of advantage where dimensional
stability is concerned. Due to the lower carbon content the
toughness is greater than the most of the other cold-work
steels. When used for cold-work tools, the steel is tempered
at 170-250°C, the resulting hardness then being 55-58
HRC. With regard to impact strength this steel, too, is susceptible
to tempering treatments around 300°C (see Figure 1).

Figure 1. Steel SIS 2550. Hardness and impact strength as
functions of tempering temperature
SIS 2550, after hardening and tempering at 200-250°C possesses
very high tensile strength and good impact strength. The values
given below have been obtained on tensile test specimens that
were oil quenched from 830°C and tempered at 250°C.
|
Rp0,02
= 1370
|
MPa
A5 = 8%
|
|
Rp0,1
= 1520
|
MPa
Z = 33%
|
|
Rp0,2 = 1630
|
MPa
HRC = 54
|
|
Rm = 2000 MPa
|
|
Such
favourable mechanical properties make the steel suitable for
tools subjected to large static and dynamic forces. Some typical
applications are dies for tableware, shear blades for heavy
plate and dies for plastic moulds, which requires steel possessing
a high degree of dimensional stability and excellent polishability.
SIS 2550
is also used for hot-work tools working at moderate temperatures,
e.g. drop-forging dies. Such tools are tempered between 400°C
and 600°C, the exact temperature depending on the hardness
required and the working temperature of the tool. For working
temperatures above approximately 400°C the hardness of
the steel falls relatively quickly.
If higher
working temperatures are involved it is recommended to use
the special hot-work steels.
Grade
S1 has both high wear resistance and high impact strength.
The hardenability is inferior to that of the Cr-Ni-Mo steel
SIS 2550. This implies that for dimensions greater than 50
mm in diameter, this steel is contour-hardening which, in
fact, further increases its toughness.
The normal
hardening temperature is about 900°C but it may be raised
to 950°C without any risk of grain growth being incurred.
If a hardness higher than 50 HRC is required in dimensions
up to about 60 mm in diameter the steel should be quenched
in oil. For heavier dimensions a combined water-oil quenching
procedure may be necessary.
Of the
many cold-work applications for tool steel, special mention
should be made of the cold punching of plate having a thickness
greater than about 3 mm. If a plate of increasing thickness
is being punched and consequently the thickness measurement
of the plate is approaching the diameter of the hole, the
punches used show an increasing tendency to break if they
are made from, for example, grades O1, A2 or D2. For this
type of punching work, grade S1 has been shown to possess
the best combination of toughness and wear resistance. A suitable
hardness is 56-58 HRC.
Wear resistance
is further increased if, during the course of the hardening
treatment, the tools are heated for some 20 min in a cyanide
bath. After this treatment no further finishing is required;
at the most a very light finish grinding is permissible. Another
example is the use of this steel as the impact hammer in nail
guns, used for driving nails into concrete.
Owing
to its high toughness in comparatively large dimensions, grade
S1 can successfully be used for tableware dies, which, depending
on their dimensions should either be quenched in oil or be
heat treated according to the combined oil-water quenching
procedure.
Another
field of application is shear blades for cold shearing of
heavy plate. Because of its rather good resistance to tempering,
grade S1 may also be used for hot shears, a suitable hardness
for this latter use being about 45 HRC.
In the
field of hot-work, grade S1 has been superseded by other grades,
e.g. H13. However, mention should be made of an interesting
and successful field of application for grade S1 -- as chisels
used in process of electrolytic reduction of Aluminium from
bauxite. The function of the chisels is to break up the hard
alumina-containing crust which forms on the metal bath. During
their use the chisels also come into contact with the bath
itself and are thus subjected to both high temperatures and
impact stresses. A suitable chisel hardness is about 350 HB.
Back
to top
Surface
Hardening of Steels
Surface
hardening a process which includes a wide variety of techniques
is used to improve the wear resistance of parts without affecting
the softer, tough interior of the part. This combination of
hard surface and resistance and breakage upon impact is useful
in parts such as a cam or ring gear that must have a very
hard surface to resist wear, along with a tough interior to
resist the impact that occurs during operation. Further, the
surface hardening of steels has an advantage over through
hardening because less expensive low-carbon and medium-carbon
steels can be surface hardened without the problems of distortion
and cracking associated with the through hardening of thick
sections.
There
are two distinctly different approaches to the various methods
for surface hardening (Table 1): methods that involve an intentional
buildup or addition of a new layer and methods that involve
surface and subsurface modification without any intentional
buildup or increase in part dimensions.
Table 1. Engineering methods for surface hardening of steels.
|
Layer
additions
|
Substrate
treatment
|
|
Hardfacing
Fusion harcifacing
Thermal spray
Coatings
Electrochemical
plating
Chemical vapor deposition (electroless plating)
Thin films (physical vapor deposition, puttering, ion
plating)
Ion mixing
|
Diffusion
methods
Carburizing
Nitriding
Carbonitriding
Nitrocarburizing
Boriding
Titanium-carbon diffusion
Toyota diffusion process
Selective
hardening methods
Flame
hardening
Induction hardening
Laser hardening
Electron beam hardening
Ion implantation
Selective carburizing and nitriding
Use of arc lamps
|
The first
group of surface hardening methods includes the use of thin
films, coatings, or weld overlays (hard-facings). Films, coatings,
and overlays generally become less cost effective as production
quantities increase, especially when the entire surface of
work pieces must be hardened.
The fatigue
performance of films, coatings, and overlays may also be a
limiting factor, depending on the bond strength between the
substrate and the added layer. Fusion-welded overlays have
strong bonds, but the primary surface-hardened steels used
in wear applications with fatigue loads include heavy case-hardened
steels and flame or induction-hardened steels. Nonetheless,
coatings and overlays can be effective in some applications.
For tool steels, for example, TiN and Al2O3 coatings are effective
not only because of their hardness but also because their
chemical inertness reduces wear and the welding of chips to
the tool. Overlays can be effective when the selective hardening
of large areas is required.
The second
group of methods on surface hardening is further divided into
diffusion methods and selective hardening methods. Diffusion
methods modify the chemical composition of the surface with
hardening species such as carbon, nitrogen, or boron. Diffusion
methods allow effective hardening of the entire surface of
a part and are generally used when a large number of parts
are to be surface hardened. In contrast, selective surface
hardening methods allow localized hardening. Selective hardening
generally involves transformation hardening (from heating
and quenching), but some selective hardening methods (selective
nitriding, ion implantation and ion beam mixing) are based
solely on compositional modification.
As previously
mentioned, surface hardening by diffusion involves the chemical
modification of a surface. The basic process used is thermo-chemical
because some heat is needed to enhance the diffusion of hardening
species into the surface and subsurface regions of part.
The depth
of diffusion exhibits time-temperature dependence such that:
Case depth
K vTime
where
the diffusivity constant, K, depends on temperature, the chemical
composition of the steel, and the concentration gradient of
a given hardening species. In terms of temperature, the diffusivity
constant increases exponentially as a function of absolute
temperature. Concentration gradients depend on the surface
kinetics and reactions of a particular process.
Methods
of hardening by diffusion include several variations of hardening
species (such as carbon, nitrogen, or boron) and of the process
method used to handle and transport the hardening species
to the surface of the part. Process methods for exposure involve
the handling of hardening species in forms such as gas, liquid,
or ions. These process variations naturally produce differences
in typical case depth and hardness (Table 2). Factors influencing
the suitability of a particular diffusion method include the
type of steel (Table 3).
It is
also important to distinguish between total case depth and
effective case depth. The effective case depth is typically
about two-thirds to three-fourths the total case depth. The
required effective depth must be specified so that the heat
treatment can process the parts for the correct time at the
proper temperature.
Table 2: Typical characteristics of diffusion treatments
| Process |
Nature
of case |
Process
temperature (°C) |
Typical
case depth |
Case
hardness (HRC) |
Typical
base metals |
| Carburizing
Pack |
Diffused
carbon |
815-1090 |
125µm-1.5mm |
50-63* |
Low-carbon
steels, low-carbon alloy steels |
Gas |
Diffused
carbon |
815-980 |
75 µm-1.5mm
|
50-63* |
Low-carbon
steels, low-carbon alloy steels |
| Liquid |
Diffused
carbon and possibly nitrogen |
815-980 |
50
µm-1.5mm |
50-65*
|
Low-carbon
steels, low-carbon alloy steels |
| Vacuum |
Diffused
carbon |
815-1090
|
75 µm-1.5mm |
50-63* |
Low-carbon steels, low-carbon alloy steels |
| Nitriding
Gas |
Diffused
nitrogen,nitrogen compounds |
480-590 |
12µm-0.75mm |
50-70 |
Alloy
steels, nitriding steels, stainless steels |
| Salt |
Diffused nitrogen, nitrogen compounds |
510-565 |
2.5µm-0.75mm |
50-70 |
Most
ferrous metals. Including cast irons |
| Ion |
Diffused nitrogen. nitrogen compounds |
340-565
|
75µm-0.75mm |
50-70 |
Alloy
steels, nitriding steels, stainless steels |
| Carbonitriding
Gas |
Diffused
carbon and nitrogen |
760-870 |
75µm-0.75mm |
50-65*
|
Low-carbon
steels, low-carbon alloy steels, stainless steels |
| Liquid
(cyaniding) |
Diffused
carbon and nitrogen |
760-870 |
2.5-125µm |
50-65*
|
Low-carbon
steels |
Ferritic nitrocarburizing |
Diffused
carbon and nitrogen |
565-675 |
2.5-25µm |
40-60* |
Low-carbon
steels |
| Other
Aluminizing (pack) |
Diffused
aluminum |
870-980 |
25µm-1mm
|
<
20 |
Low-carbon
steels |
| Siliconizing
by chemical vapor deposition |
Diffused
silicon |
925-1040
|
25µm-1mm |
30-50 |
Low-carbon
steels |
| Chromizing
by chemical vapor deposition |
Diffused
chromium |
980-1090 |
25-50µm |
Low-carbon
steel < 30; High-carbon 50-60 |
High- and low carbon steels |
| Titanium
Carbide |
Diffused
carbon and titanium, TiC compound |
900-1010 |
2,5-12.5µm |
>
70* |
Alloy
steels, tool steels |
*
Requires quench from austenitizing temperature.
Table
3. Types of steels used for various diffusion processes
|
Diffusion
substrates
|
|
Low-carbon
steels
|
Alloy
steels
|
Tool
steels
|
Stainless
steels
|
Carburizing
Cyaniding
Ferritic nitrocarburizing
Carbonitriding |
Nitriding
Ion nitriding |
Titanium
carbide
Boriding
Salt nitriding
Ion nitriding
Gas nitriding |
Gas
nitriding
Titanium carbide
Ion nitriding
Ferritic nitrocarburizing |
Back
to top
Carburizing
Carburizing
is the addition of carbon to the surface of low-carbon steels
at temperatures generally between 850 and 950°C (1560
and 1740°F), at which austenite, with its high solubility
for carbon, is the stable crystal structure. Hardening is
accomplished when the high-carbon surface layer is quenched
to form martensite so that a high-carbon martensitic case
with good wear and fatigue resistance is superimposed on a
tough, low-carbon steel core.
Case
hardness of carburized steels is primarily a function of carbon
content. When the carbon content of the steel exceeds about
0.50% additional carbon has no effect on hardness but does
enhance hardenability. Carbon in excess of 0.50% may not be
dissolved, which would thus require temperatures high enough
to ensure carbon-austenite solid solution.
Case
depth of carburized steel is a function of carburizing time
and the available carbon potential at the surface. When prolonged
carburizing times are used for deep case depths, a high carbon
potential produces a high surface-carbon content, which may
thus result in excessive retained austenite or free carbides.
These two microstructural elements both have adverse effects
on the distribution of residual stress in the case-hardened
part. Consequently, a high carbon potential may be suitable
for short carburizing times but not for prolonged carburizing.
Carburizing
steels for case hardening usually have base-carbon contents
of about 0.2%, with the carbon content of the carburized layer
generally being controlled at between 0.8 and 1% C. However,
surface carbon is often limited to 0.9% because too high a
carbon content can result in retained austenite and brittle
martensite.
Most
steels that are carburized are killed steels (deoxidized by
the addition of aluminum), which maintain fine grain sizes
to temperatures of about 1040°C. Steels made to coarse
grain practices can be carburized if a double quench provides
grain refinement. Double quenching usually consists of a direct
quench and then a requench from a lower temperature.
Many
alloy steels for case hardening are now specified on the basis
of core hardenability. Although the same considerations generally
apply to the selection of uncarburized grades, there are some
peculiarities in carburizing applications.
First,
in a case-hardened steel, the hardenability of both case and
core must be considered. Because of the difference in carbon
content, case and core have quite different hardenabilities,
and this difference is much greater for some steels than for
others.
Moreover,
the two regions have different in-service functions to perform.
Until the introduction of lean alloy steels such as the 86xx
series, with and without boron, there was little need to be
concerned about case hardenability because the alloy content
combined with the high carbon content always provided adequate
hardenability. This is still generally true when the steels
are direct quenched from carburizing, so that the carbon and
alloying elements are in solution in the case austenite. In
parts that are reheated for hardening and in heavy-sectioned
parts, however, both case and core hardenability requirements
should be carefully evaluated.
The
relationship between the thermal gradient and the carbon gradient
during quenching of a carburized part can make a measurable
difference in the case depth as measured by hardness. That
is, an increase in base hardenability can produce a higher
proportion of martensite for a given carbon level, yielding
an increased measured case depth. Therefore, a shallower carbon
profile and shorter carburizing time could be used to attain
the desired result in a properly chosen steel.
Core
Hardness. A common mistake is to specify too narrow a range
of core hardness. When the final quench is from a temperature
high enough to allow the development of full core hardness,
the hardness variation at any location will be that of the
hardenability band of the steel at the corresponding position
on the end-quenched hardenability specimen.
In
standard steels purchased to chemical composition requirements
rather than to hardenability, the range can be 20 or more
HRC points; for example, 8620 may vary from 20 to 45 HRC at
the 4/16 in.(6.35mm) position. The 25-point range emphasizes
the advantage of purchasing to hardenability specifications
to avoid the intolerable variation possible within the ranges
for standard chemistry steels. Another way to control core
hardness within narrow limits without resorting to the use
of high-alloy steels is to use a final quench from a lower
temperature so that full hardness in the case will be developed
without the disadvantage of excessive core hardness.
Gears
are almost always oil quenched because distortion must be
held to the lowest possible level. Therefore, alloy steels
are usually selected, with much debate about which particular
alloy. The lower-alloy steels such as 4023, 5120, 4118, 8620,
and 4620, with a carbon range between 0.15 and 0.25%, are
widely used and generally satisfactory. Usually, the first
choice is one of the last two steels mentioned, either of
which should be safe for all ordinary applications. The final
choice, based on service experience or dynamometer testing,
should be the least expensive steel that will do the job.
For heavy-duty applications, higher-alloy grades such as 4320,
4817, and 9310 are justifiable if based on actual performance
tests. The life testing of gears in the same mountings used
in service to prove both the design and the steel selection
is particularly important.
In
other applications, when distortion is not a major factor,
the carbon steels described above, water quenched, can be
used up to a 50 mm (2 in.) diameter. In larger sizes, low-alloy
steels, water quenched, such as 5120, 4023, and 6120 can be
used, but possible distortion and quench cracking must be
avoided.
Carburizing
Methods. While the basic principle of carburizing has remained
unchanged since carburizing was first employed, the method
used to introduce the carbon into the steel has been a matter
of continuous evolution.
In
its earliest application, parts were simply placed in a suitable
container and covered with a thick layer of carbon powder
(pack carburizing). Although effective in introducing carbon,
this method was exceedingly slow, and as the demand for greater
production grew, a new process using a gaseous atmosphere
was developed.
In
gas carburizing, the parts are surrounded by a carbon-bearing
atmosphere that can be continuously replenished so that a
high carbon potential can be maintained. While the rate of
carburizing is substantially increased in the gaseous atmosphere,
the method requires the use of a multicomponent atmosphere
whose composition must be very closely controlled to avoid
deleterious side effects, for example, surface and grain-boundary
oxides. In addition, a separate piece of equipment is required
to generate the atmosphere and control its composition. Despite
this increased complexity, gas carburizing has become the
most effective and widely used method for carburizing steel
parts in large quantities.
In
efforts required to simplify the atmosphere, carburizing in
an oxygen-free environment at very low pressure (vacuum carburizing)
has been explored and developed into a viable and important
alternative. Although the furnace enclosure in some respects
becomes more complex, the atmosphere is greatly simplified.
A single-component atmosphere consisting solely of a simple
gaseous hydrocarbon, for example methane, may be used. Furthermore,
because the parts are heated in an oxygen-free environment,
the carburizing temperature may be increased substantially
without the risk of surface or grain-boundary oxidation. The
higher temperature permitted increases not only the solid
solubility of carbon in the austenite but also its rate of
diffusion, so that the time required to achieve the case depth
desired is reduced.
Although
vacuum carburizing overcomes some of the complexities of gas
carbunzing, it introduces a serious new problem that must
be addressed. Because vacuum carburizing is conducted at very
low pressures, and the rate of flow of the carburizing gas
into the furnace is very low, the carbon potential of the
gas in deep recesses and blind holes is quickly depleted.
Unless this gas is replenished, a great nonuniformity in case
depth over the surface of the part is likely to occur. If,
in an effort to overcome this problem, the gas pressure is
increased significantly, another problem arises, that of free-carbon
formation, or sooting.
Thus,
in order to obtain cases of reasonably uniform depth over
a part of complex shape, the gas pressure must be increased
periodically to replenish the depleted atmosphere in recesses
and then reduced again to the operating pressure. Clearly,
a delicate balance exists in vacuum carburizing: The process
conditions must be adjusted to obtain the best compromise
between case uniformity, risk of sooting, and carburizing
rate.
A
method that overcomes both of these major problems, yet retains
the desirable features of a simple atmosphere and permissible
operating temperature is plasma or ion carburizing.
To
summarize, carburizing methods include:
Gas
carburizing
Vacuum carburizing
Plasma carburizing
Salt bath carburizing
Pack carburizing
These methods introduce carbon by the use of gas (atmospheric-gas,
plasma, and vacuum carburizing), liquids (salt bath carburizing),
or solid compounds (pack carburizing). All of these methods
have limitations and advantages, but gas carburizing is used
most often for large-scale production because it can be accurately
controlled and involves a minimum of special handling.
Vacuum carbunzing and plasma carburizing have found applications
because of the absence of oxygen in the furnace atmosphere.
Salt bath and pack carburizing arc still done occasionally,
but have little commercial importance today.
Process
characteristics of the above-mentioned carburizing methods
fall into two general groups:
Conventional
methods, which introduce carbon by gas atmospheres, salt baths
or charcoal packs
Plasma methods, which impinge positive carbon ions on the
surface of a steel part (the cathode)
The main difference between conventional and plasma methods
is the reduced carburizing times achieved in plasma-assisted
methods. The quickly attained surface saturation also results
in faster diffusion kinetics. Furthermore, plasma carburizing
produces very uniform case depths, even in parts with irregular
surfaces.
With the conventional methods, carburization always takes
place by means of a gaseous phase of carbon monoxide; however,
each method also involves different reaction and surface kinetics,
producing different case-hardening results.
In
general, with conventional methods, carbon monoxide breaks
down at the steel surface:
2CO
? CO2 + C
The
liberated carbon is readily dissolved by the austenite phase
and diffuses into the body of the steel. For some process
methods (gas and pack carburizing), the carbon dioxide produced
may react with the carbon atmosphere or pack charcoal to produce
new carbon monoxide by the reverse reaction.
Carburizing
is most frequently performed between 850 and 950°C (1550
and 1750°F), but sometimes higher temperatures are used
to reduce cycle times and/or produce deeper depths of the
high-carbon surface layer.
A
comprehensive model of gas carburization must include algorithms
that describe:
Carbon
diffusion
Kinetics of the surface reaction
Kinetics of the reaction between endogas and enriching gas
Purging (for batch processes)
The atmosphere control system.
Back
to top
Nitriding
Nitriding
is a surface-hardening heat treatment that introduces nitrogen
into the surface of steel at a temperature range (500 to 550°C,
or 930 to 1020°F), while it is in the ferrite condition.
Thus, nitriding is similar to carburizing in that surface
composition is altered, but different in that nitrogen is
added into ferrite instead of austenite. Because nitriding
does not involve heating into the austenite phase field and
a subsequent quench to form martensite, nitriding can be accomplished
with a minimum of distortion and with excellent dimensional
control.
The mechanism
of nitriding is generally known, but the specific reactions
that occur in different steels and with different nitriding
media are not always known. Nitrogen has partial solubility
in iron. It can form a solid solution with ferrite at nitrogen
contents up to about 6%. At about 6% N, a compound called
gamma prime (?), with a composition of Fe4N is formed.
At nitrogen
contents greater than 8%, the equilibrium reaction product
is e compound, Fe3N. Nitrided cases are stratified. The outermost
surface can be all ? and if this is the case, it is
referred to as the white layer. Such a surface layer is undesirable:
it is very hard profiles but is so brittle that it may spall
in use. Usually it is removed; special nitriding processes
are used to reduce this layer or make it less brittle. The
e zone of the case is hardened by the formation of the Fe3N
compound, and below this layer there is some solid solution
strengthening from the nitrogen in solid solution.
Principal
reasons for nitriding are:
To obtain
high surface hardness
To increase wear resistance
To improve fatigue life
To improve corrosion resistance (except for stainless steels)
To obtain a surface that is resistant to the softening effect
of heat at temperatures up to the nitriding temperature
Nitridable Steels
Nitrided steels are generally medium-carbon (quenched and
tempered) steels that contain strong nitride-forming elements
such as aluminum, chromium, vanadium, and molybdenum.
The most significant hardening is achieved with a class of
alloy steels (nitralloy type) that contain about 1% Al. When
these steels are nitrided the aluminum forms AlN particles,
which strain the ferrite lattice and create strengthening
dislocations. Titanium and chromium are also used to enhance
case hardness although case depth decreases as alloy content
increases.
Of the
alloying elements commonly used in commercial steels, aluminum,
chromium, vanadium, tungsten and molybdenum are beneficial
in nitriding because they form nitrides that are stable at
nitriding temperatures. Molybdenum in addition to its contribution
as a nitride former also reduces the risk of embrittlement
at nitriding temperatures. Other alloying elements such as
nickel, copper, silicon and manganese have little, if any,
effect on nitriding characteristics.
Although
at suitable temperatures all steels are capable of forming
iron nitrides in the presence of nascent nitrogen, the nitriding
results are more favorable in those steels that contain one
or more of the major nitride-forming alloying elements. Because
aluminum is the strongest nitride former of the common alloying
elements, aluminum containing steels (0.85 to 1.50% Al) yield
the best nitriding results in terms of total alloy content.
The
following steels can be gas nitrided for specific applications:
Aluminum-containing
low-alloy steels
Medium-carbon, chromium-containing low-alloy steels of the
4100, 4300, 5100, 6100, 8600, 8700 and 9800 series
Hot-work die steels containing 5% chromium such as HI1, HI2,
and HI3
Low-carbon, chromium-containing low-alloy steels of the 3300,
8600, and 9300 series
Air-hardening tool steels such as A-2, A-6, D-2, D-3 and S-7
High-speed tool steels such as M-2 and M-4
Nitronic stainless steels such as 30, 40, 50, and 60
Ferritic and martensitic stainless steels of the 400 and 500
series
Austenitic stainless steels of the 200 and 300 series
Precipitation-hardening stainless steels such as 13-8 PH,
15-5 PH, 17-4 PH, 17-7 PH, A-286, AM350 and AM355.
Nitriding processes
Process methods for nitriding include:
gas (box furnace or fluidized bed),
liquid (salt bath),
plasma (ion) nitriding.
The advantages and disadvantages of these techniques are similar
to those of carburizing. However, times for gas nitriding
can be quire long, that is, from 10 to 130 h depending on
the application, and the case depths are relatively shallow,
usually less than 0.5 mm. Plasma nitriding allows faster nitriding
times, and the quickly attained surface saturation of the
plasma process results in faster diffusion. Plasma nitriding
can also clean the surface by sputtering.
Gas
Nitriding
Gas nitriding is a case-hardening process whereby nitrogen
is introduced into the surface of a solid ferrous alloy by
holding the metal at a suitable temperature in contact with
a nitrogenous gas, usually ammonia. Quenching is not required
for the production of a hard case. The nitriding temperature
for all steels is between 495 and 565°C.
Because of the absence of a quenching requirement with attendant
volume changes, and the comparatively low temperatures employed
in this process, nitriding of steels produces less distortion
and deformation than either carburizing or conventional hardening.
Some growth occurs as a result of nitriding but volumetric
changes are relatively small.
Prior
Heat Treatment. All hardenable steels must be hardened and
tempered before being nitrided. The tempering temperature
must be high enough to guarantee structural stability at the
nitriding temperature: the minimum tempering temperature is
usually at least 30°C (50°F) higher than the maximum
temperature to be used in nitriding.
Single-Stage
and Double-Stage Nitriding. Either a single- or a double-stage
process may be employed when nitriding with anhydrous ammonia.
In the single-stage process, a temperature in the range of
about 495 to 525°C is used and the dissociation rate ranges
from 15 to 30%. This process produces a brittle nitrogen-rich
layer known as the white nitride layer at the surface of the
nitrided case.
The double-stage
process, known also as the Floe process, has the advantage
of reducing the thickness of the white nitrided layer.
The first
stage of the double-stage process is, except for time, a duplication
of the single-stage process. The second stage may proceed
at the nitriding temperature employed for the first stage
or the temperature may be increased to from 550 to 565°C;
however, at either temperature, the rate of dissociation in
the second stage is increased to 65 to 80% (preferably 75
to 80%). Generally, an external ammonia dissociator is necessary
for obtaining the required higher second-stage dissociation.
The principal
purpose of double-stage nitriding is to reduce the depth of
the white layer produced on the surface of the case. Except
for a reduction in the amount of ammonia consumed per hour,
there is no advantage in using the double-stage process unless
the amount of white layer produced in single-stage nitriding
cannot be tolerated on the finished part or unless the amount
of finishing required after nitriding is substantially reduced.
To summarize,
the use of a higher temperature during the second stage:
Lowers
the case hardness
Increases the case depth
May lower the core hardness depending on the prior tempering
temperature and the total nitriding cycle time
May lower the apparent effective case depth because of the
loss of core hardness depending on how effective case depth
is defined.
Operating Procedures. After hardening and tempering and before
nitriding, parts should be thoroughly cleaned. Most parts
can be successfully nitrided immediately after vapor degreasing.
Bright
Nitriding
Bright nitriding is a modified form of gas nitriding employing
ammonia and hydrogen gases. Atmosphere gas is continually
withdrawn from the nitriding furnace and passed through a
temperature-controlled scrubber containing a water solution
of sodium hydroxide (NaOH). Trace amounts of hydrogen cyanide
(HCN) formed in the nitriding furnaces are removed in the
scrubber thus improving the rate of nitriding.
The scrubber also establishes a predetermined moisture content
in the nitriding atmosphere reducing the rate of cyanide formation
and inhibiting the cracking of ammonia to molecular nitrogen
and hydrogen. By this technique control over the nitrogen
activity of the furnace atmosphere is enhanced and nitrided
parts can be produced with little or no white layer at the
surface. If present, the white layer will be composed of only
the more ductile Fe4N (gamma prime) phase.
Pack Nitriding
Pack nitriding is a process analogous to pack carburizing.
It employs certain nitrogen-bearing organic compounds as a
source of nitrogen. Upon heating, the compounds used in the
process form reaction products that are relatively stable
at temperatures up to 570°C.
Slow decomposition of the reaction products at the nitriding
temperature provides a source of nitrogen. Nitriding times
of 2 to 16 h can be employed. Pans are packed in glass ceramic
or aluminum containers with the nitriding compound, which
is often dispersed in an inert packing media.
Ion (or Plasma) Nitriding
Since the mid-1960s, nitriding equipment utilizing the glow-discharge
phenomenon has been commercially available. Initially termed
glow-discharge nitriding, the process is now generally known
as ion, or plasma, nitriding. The term plasma nitriding is
gaining acceptance.
Ion nitriding is an extension of conventional nitriding processes
using plasma-discharge physics. In vacuum, high-voltage electrical
energy is used to form a plasma, through which nitrogen ions
are accelerated to impinge on the workpiece. This ion bombardment
heats the workpiece, cleans the surface, and provides active
nitrogen.
Metallurgically
versatile, the process provides excellent dimensional control
and retention of surface finish. Ion nitriding can be conducted
at temperatures lower than those conventionally employed.
Control of white-layer composition and thickness enhances
fatigue properties. The span of ion-nitriding applications
includes conventional ammonia- gas nitriding, short-cycle
nitriding in salt bath or gas, and the nitriding of stainless
steels.
Ion nitriding
lends itself to total process automation, ensuring repetitive
metallurgical results. The absence of pollution and insignificant
gas consumption are important economic and public policy factors.
Moreover, selective nitriding accomplished by simple masking
techniques may yield significant economies.
Comparison of Ion Nitriding and Ammonia-Gas Nitriding
Ammonia-gas nitriding produces a compound zone that is a mixture
of both epsilon and gamma-prime structures. High internal
stresses result from differences in volume growth associated
with the formation of each phase. The interfaces between the
two crystal structures are weak. Thicker compound zones, formed
by ammonia-gas nitriding, limit accommodation of the internal
stresses resulting from the mixed structure.
Under cyclic loading, cracks in the compound zone can serve
as initiation points for the propagation of fatigue cracks.
The single-phase gamma-prime compound zone, which is thin
and more ductile, exhibits superior fatigue properties. Reducing
the thickness of the ion-nitrided compound zone further improves
fatigue performance. Maximization occurs at the limiting condition,
where compound zone depth equals zero.
Case Hardness.
The bulk of the thickness of the nitride case is the diffusion
zone where fine iron/alloy nitride precipitates impart increased
hardness and strength. Compressive stresses are also developed,
as in other nitriding processes. Hardness profiles resulting
from ion nitriding are similar to ammonia-gas nitriding but
near-surface hardness may be greater with ion nitriding, a
result of lower processing temperature.
Advantages
and Disadvantages of Ion Nitriding. Ion nitriding achieves
repetitive metallurgical results and complete control of the
nitrided layers. This control results in superior fatigue
performance, wear resistance, and hard layer ductility. Moreover,
the process ensures high dimensional stability, eliminates
secondary operations, offers low operating-temperature capability
and produces parts that retain surface finish.
Among
operating benefits are:
Total
absence of pollution
Efficient use of gas and electrical energy
Total process automation
Selective nitriding by simple masking techniques
Process span that encompasses all sub-critical nitriding
Reduced nitriding time
The limitations of ion nitriding include high capital cost,
need for precision fixturing with electrical connections,
long processing times compared to other short-cycle nitrocarburizing
processes, and lack of feasibility of liquid quenching for
carbon steels.
Bck
to top
The
Tempering of Martensite
Martensite
is a very strong phase but it is normally very brittle so
it is necessary to modify the mechanical properties by heat
treatment in the range 150-700°C. This process, which
is called tempering, is one of the oldest heat treatments
applied to steels although it is only in recent years that
a detailed understanding of the phenomena involved has been
reached.
Essentially,
martensite is a highly supersaturated solid solution of carbon
in iron, which, during tempering, rejects carbon in the form
of finely divided carbide phases. The end result of tempering
is a fine dispersion of carbides in an a-iron matrix, which
often bears little structural similarity to the original as-quenched
martensite.
It should
be noted that, in many steels, the martensite reaction does
not go to completion on quenching, resulting in varying amounts
of retained austenite which does not remain stable during
the tempering process.
Tempering of plain carbon steels
The as-quenched martensite possesses a complex structure.
This occurs in the first-formed martensite, i.e. the martensite
formed near Ms, which has the opportunity of tempering during
the remainder of the quench. This phenomenon, which is referred
to as auto-tempering, is clearly more likely to occur in steels
with a high Ms.
On reheating as-quenched martensite, the tempering takes place
in four distinct but overlapping stages:
up to
250°C, precipitation of a-iron carbide; partial loss of
tetragonality in martensite
between 200 and 300°C, decomposition of retained austenite
between 200 and 350°C, replacement of a-iron carbide by
cementite; martensite loses tetragonality
above 350°C, cementite coarsens and spheroidizes; recrystallization
of ferrite.
Tempering
stage 1
Martensite formed in medium and high carbon steels (0.3-1.5%
C) is not stable at room temperature because interstitial
carbon atoms can diffuse in the tetragonal martensite lattice
at this temperature. This instability-increases between room
temperature and 2500°C, when iron carbide precipitates
in the martensite.
Tempering
stage 2
During stage 2, austenite retained during quenching is decomposed,
usually in the temperature range 230-300°C. Cohen and
coworkers detected this stage by X-ray diffraction measurements
as well as dilatometric and specific volume measurements.
However, the direct observation of retained austenite in the
microstructure has always been rather difficult, particularly
if it is present in low concentrations. The little available
evidence suggests that in the range 230-300°C, retained
austenite decomposes to bainite, ferrite and cementite, but
no detailed comparison between this phase and lower bainite
has yet been made.
Tempering
stage 3
During the Third stage of tempering, cementite first appears
in the microstructure as a Widmanstatten distribution of rods,
which have a well-defined orientation relationship with the
matrix which has now lost its tetragonality and become ferrite.
This reaction commences as low as 100°C, and is fully
developed at 300°C, with particles up to 200 nm long and
~15 nm in diameter. Similar structures are often observed
in lower carbon steels as quenched, as a result of the formation
of Fe3C during the quench. During tempering, the replacement
of transition carbides and low-temperature martensite by cementite
and ferrite.
During
the third stage of tempering the tetragonality of the matrix
disappears and it is then, essentially, ferrite, not supersaturated
with respect to carbon. Subsequent changes in the morphology
of the cementite particles occur by an Ostwald ripening type
of process, where the smaller particles dissolve in the matrix
providing carbon for the selective growth of the larger particles.
Tempering stage 4
It is useful to define a fourth stage of tempering in which
the cementite particles undergo a coarsening process and essentially
lose their crystallographic morphology, becoming spheroidized.
The coarsening commences between 300 and 400°C, while
spheroidization takes place increasingly up to 700°C.
At the higher end of this range of temperature the martensite
lath boundaries are replaced by more equiaxed ferrite grain
boundaries by a process which is best described as recrystallization.
The final result is an equiaxed array of ferrite grains with
coarse spheroidized particles of Fe3C partly, but not exclusively,
in the grain boundaries.
The spheroidization of the Fe3C rods is encouraged by the
resulting decrease in surface energy. The particles, which
preferentially grow and spheroidize are located mainly at
interlath boundaries and prior austenite boundaries, although
some particles remain in the matrix. The boundary sites are
preferred because of the greater ease of diffusion in these
regions. The original martensite lath boundaries remain stable
up to about 600°C, but in the range 350-600°C, there
is considerable rearrangement of the dislocations within the
laths and at those lath boundaries which are essentially low
angle boundaries.
Role of carbon content
Carbon has a profound effect on the behavior of steels during
tempering. Firstly, the hardness of the as-quenched martensite
is largely influenced by the carbon content, as is the morphology
of the martensite laths which have a {111} habit plane up
to 0.3 % C, changing to {225} at higher carbon contents.
The Ms temperature is reduced as the carbon content increases,
and thus the probability of the occurrence of auto-tempering
is less. During fast quenching in alloys with less than 0.2
% C, the majority (up to 90%) of the carbon segregates to
dislocations and lath boundaries, but with slower quenching
some precipitation of cementite occurs.
On subsequent
tempering of low carbon steels up to 200°C further segregation
of carbon takes place, but no precipitation has been observed.
Under normal circumstances it is difficult to detect any tetragonality
in the martensite in steels with less than 0.2 % C, a fact
which can also be explained by the rapid segregation of carbon
during quenching.
Mechanical properties of tempered plain carbon steels
The intrinsic mechanical properties of tempered plain carbon
martensitic steels are difficult to measure for several reasons.
Firstly, the absence of other alloying elements means that
the hardenability of the steels is low, so a fully martensitic
structure is only possible in thin sections. However, this
may not be a disadvantage where shallow hardened surface layers
are all that is required. Secondly, at lower carbon levels,
the Ms temperature is rather high, so tempering is likely
to take place. Thirdly, at the higher carbon levels the presence
of retained austenite will influence the results. Added to
these factors, plain carbon steels can exhibit quench cracking
which makes it difficult to obtain reliable test results.
This is particularly the case at higher carbon levels, i.e.
above 0.5% carbon.
Provided care is taken, very good mechanical properties, in
particular proof and tensile stresses, can be obtained on
tempering in the range 100-300°C. However, the elongation
is frequently low and the impact values poor. Plain carbon
steels with less than 0.25% C are not normally quenched and
tempered, but in the range 0.25-0.55 % C heat tr
|