Module 37
Surface hardening
Lecture 37
Surface hardening
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NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
Keywords : Non‐uniform properties in engineering components, methods of surface hardening, shot peening, hard facing, induction hardening, surface modification by diffusion, carburizing, post carburizing heat treatment, core refining, case hardening, origin of residual stress, nitriding, Fe‐N phase diagram, effect of surface hardening on fatigue resistance of engineering components
Introduction
The last six lectures were devoted to heat treatment of steel. We have seen that hardening followed by tempering gives the best combination of strength and toughness. Formation of martensite is primarily responsible for the development of very high strength in steel. However you need to cool a component made of steel very fast to get martensite both at its surface and at its centre. Although it may be rather easy to achieve a high cooling rate at the surface but maintaining a high cooling rate at the centre may be extremely difficult particularly if the section size of the component is large. Therefore the microstructure at the centre of a thick section is likely to be different from that at its surface. There are several applications where we do not need uniform microstructure or property across the section. For example components like turbine shaft, gear, spindle and axle need to have a hard surface but a soft core. In general high strength means low toughness. If the section size of a component is too high to be fully hardened we may still have a soft core. It might be one of the methods of fulfilling such a criterion. There are several other ways the strength or the hardness of the surface can be increased without adversely affecting the toughness of the core. Some of the most common techniques are as follows:
Induction hardening Case carburizing + case hardening Nitriding Shot peening Hard facing, coating or surface alloying
In this module we shall learn about some of these. The properties of steel or any other engineering material depend a great deal on the processing route that is followed and its composition. For example we know that cast metals have coarse inhomogeneous grains with preferred orientation. Subsequent processing consisting of homogenization, forging, rolling and annealing may result in a uniform fine grain structure having isotropic properties. As a result there may be a substantial improvement in its strength and ductility. In the case of steel the possible options are much more varied. In short all materials may 2 have an inherent base property or microstructure which can be altered or improved by adopting an appropriate processing route. The performance of a component depends
NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
primarily on the properties of the material of which it is made. The interrelation between the four is best described by the tetrahedron shown in fig 1.
Performance
Processing: Properties micrstructure
Material Fig 1: Tetrahedron showing the interrelation between material, its processing route and its property on the performance of a component.
Non‐uniform properties in engineering components:
It is extremely difficult to have a uniform microstructure within a material unless it is extremely thin. This is because the evolution of microstructure within a material depends on the local processing parameters. Often it is difficult to maintain identical conditions at every point within a material unless it is extremely thin. The effect is more pronounced in the case of steel that goes through a solid state transformation during cooling. The cooling rate within a component is a strong function of its section size. It is impossible to maintain identical cooling rate within a component of finite dimension. Therefore we have to live with non‐uniform properties in engineering components since it cannot be avoided in components of reasonable thickness. This is illustrated with the help of an example in slide 1.
Steel I beam is one of the most common structural components. A cross section of I beam is shown in slide 1. Its flange which is highly stressed is thick but its web where the stress is not so high is relatively thin. I beams are made by hot rolling at a temperature while the structure of steel is austenite. On completion of rolling I beam is allowed to cool in air. The average cooling curves of the flange and the web of the beam have been super imposed on the CCT diagram of 0.2%C steel. The cooling rate within the web is a little faster than that in the flange. Therefore 3 the microstructure of the web is likely to be finer than that in the flange. It is likely to have relatively less %ferrite but more %pearlite in comparison to those in the flange. The web is therefore expected to be stronger than the flange although it is not necessary to make it
NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
stronger. Here is an application where the differential properties of an engineering component are not being properly exploited. There are several other uses where intentionally the structure of the material is altered either by local change in composition or by local deformation or by adopting differential cooling rates at different places so as to improve its performance as an engineering component. We would look at a few such examples.
Non uniform properties in engineering components I beam A3 flange A1 + P web T Flange Slide 1 web Web: least stressed: thin Ms + M Flange: high stress: thick time I Beam: hot rolled sections Case: where we have % C ~ 0.2 to learn to live with it. Surface hardening: Which is stronger ? exploit such features.
Surface hardening: why & how?
Components like gear, shaft or spindle need a hard / wear resistant surface but a soft / tough core. Section size of such components is often too large to be uniformly hardened even on severe quenching. More over the time lag between the transformations at the surface and the core results in an unfavorable tensile residual stress at the surface. Recall the general thumb rule that the region that transforms later is likely to have compressive residual stress. The surface is likely to transform first in steel having the same composition all through its section. Therefore surface would have residual tensile stress. Depending on its magnitude it may lead to cracking or distortion. The presence of residual tensile stress is also harmful as it would reduce fatigue life of critical components like turbine shaft or landing gear of an aircraft. The purpose 4 of surface hardening is to develop a hard surface with compressive residual stress, to improve its wear resistance, to increase its fatigue life and to avoid susceptibility to distortion and cracking. The most commonly used methods of surface hardening are as follows:
NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
• Shot peening: general applicable to all metals • Coating / hard facing • Surface (local) heating & cooling: steel • Surface diffusion & subsequent treatment
Shot peening:
Shot peening technique is applicable to all metals and alloys that are amenable to plastic deformation. The part to be hardened is placed in a chamber where extremely fine hard particles moving at a high speed keep striking at its surface. The energy of the moving particles is high enough to cause local plastic deformation at its surface. The stress on the material a little beneath the surface is not high enough to cause plastic deformation. However it would be under elastic stress as long as the shot peening process continues. When it stops residual stress would develop at the surface because of the elastic recovery that occurs in the region a little beneath the surface. Proper control on the process parameters such as the particle size, its kinetic energy, the angle of incidence and the time may be necessary to develop favorable residual stress pattern at the surface. It is compressive in nature. Therefore it would inhibit crack initiation. Landing gears of aircrafts are subjected to shot peening to develop residual compressive stress on its surface. Even automotive gears, following carburizing, are subjected shot peening to raise the value of compressive residual stress (to as high as 1000 – 1200 MPa), particularly at depths of 30 – 40 microns. This help resist crack propagation during service as result of fatigue loading.
Hard facing:
Engineering components that are required to resist solid particle erosion, abrasion, fretting or cavitation are usually given a hard surface coating. This consists of a fine dispersion of hard metal carbides in a compatible metal matrix. Thermal spray is the most commonly used technique to apply such coatings on the component. There are specially designed setups with spray guns that suck the coating material along with oxygen and fuel gas that ignites into a flame to melt the matrix of the coating material while it deposits on the surface of the component. The most commonly used coating materials are mixtures of chromium or tungsten carbides in either cobalt or nickel‐chromium alloy matrix. Hard facing is also a commonly used technique to salvage worn out parts so that they could be reused.
Induction hardening: a method based on local heating followed by cooling:
5 This is applicable only for steel. An induction coil is used to heat the component to be hardened. Only the surface gets heated. Its microstructure transforms into austenite from a mixture of ferrite and cementite, but the structure of the core remains intact as it remains cold
NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
all through the process. Once the temperature of the surface attains a specified level the power is switched off and the job is cooled rapidly by quenching it in water. Heat extraction rate is much faster than that in a conventional hardening process. This is because only a thin region near the surface of the component gets heated. The total amount of heat stored is so less that it can be easily extracted by the quenching medium. The centre of the component does not get heated at all. The cold core acts as a sink for the heat stored within the thin region near the surface. Thus it also helps attain a very high cooling rate at the surface. Once the process is complete the microstructure of the surface gets transformed into martensite while that at its core remains unaltered. Induction heating is extremely fast and the time the
component spends above A3 temperature is very short. Therefore to ensure complete transformation of ferrite to austenite the peak temperature should be a little higher than the normal austenitizing temperature used for conventional hardening heat treatment. The total
time spent above A3 may still not be long enough to have homogeneous austenite within the entire hot section. The composition of martensite nucleating in inhomogeneous austenite may vary. Therefore hardness of induction hardened steel component may often be higher than that in through hardened steel having identical composition. One of the main advantages of induction hardening is good surface finish and little distortion. It can be applied to all grades of steel. Alloy addition is not necessary. Induction hardening is very effective for surface hardening of plain carbon steel having 0.35‐0.70%C. The salient features of induction hardening are as follows:
• Heat the surface to a temperature above A3 (austenitic region) • Core does not get heated : the structure remains unaltered • Surface converts to martensite on quenching. • Fast heating & short hold time: needs higher austenization temperature • Martensite forms in fine inhomogeneous grains of austenite • Applicable to carbon steels (0.35 – 0.7C) • Little distortion & good surface finish
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NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
Induction hardening Place the job inside an induction coil & pass high frequency ac. Surface gets heated due to skin effect. Job High Heating: local surface near Coil AC the coil gets heated = resistivity Slide 2 = frequency d = magnetic permeability Higher frequency: lower depth of hardening (d). On quenching only surface becomes martensite.
Slide 2 shows with the help of a diagram the setup needed for induction hardening. It consists of a high frequency AC power source and water cooled induction coil surrounding the job to be hardened. Only the surface gets heated due to skin effect. The expression for the depth of penetration of the field is given in slide 2. It depends on the frequency of power source, the resistivity (increases with temperature) and the magnetic permeability of steel (It decreases significantly as the temperature goes beyond Curie point). There will be a sudden increase in d as the temperature goes beyond 750°C. The only parameter that can be controlled is the frequency. Higher the frequency lower is the depth of penetration. You could select a lower frequency to get a higher depth of hardening.
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NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
Structure & properties Homogeneous T for Sph austenite Grain Ann growth
Plate (HC) T T martensite Needs %C time Much higher austenitization time Slide 3 tempering required as hold time is short Cm globules Spheroidising annealing is done in matrix before induction hardening Spheroidising Hard surface & tough core. annealing Compressive residual stress at surface & tensile at core
Slide 3 explains with the help of a set of diagrams what should be the ideal microstructure at the surface (or the case) and the core of a component and how these can be attained. The case preferably should have high carbon martensite to ensure the maximum possible hardness. The core on the other hand should have globular cementite in a matrix of ferrite. This is the structure that has the highest toughness. Such a microstructure can be developed in steel by
prolonged soaking (thermal exposure) at a temperature a little below A1 (eutectoid temperature). The process is known as spheroidising annealing. The appropriate temperature range for spheroidising annealing has been marked on the phase with the help of a filled rectangle. It denotes the range of temperature and composition of steel suitable for induction
hardening. If the temperature keeps oscillating around A1 the process of spheroidization is faster. Spheroidizing annealing should always precede induction hardening.
The peak temperature to be used for induction hardening of eutectoid steel has been marked with the help of a solid (filled) circle on the phase diagram given in slide 3. This is much higher than 760°C. There is a time temperature transformation diagram for austenitization just beside the phase diagram in slide 3. Note that the hold time at this temperature is not long enough to form homogeneous austenite. It means %C in austenite may not be the same at all places. This suggests that on quenching, martensite would nucleate within inhomogeneous austenite. This is accompanied by volume expansion. However the core beneath it would not let it happen. As a result there residual compressive stress would develop at the surface. This inhibits nucleation 8 of surface crack. However martensite is brittle. It may be surrounded by retained austenite as well. Therefore induction hardening must be followed by tempering.
NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
Surface diffusion & subsequent treatment:
The main objective of surface hardening is to have a hard surface but a soft core. Recall that the hardness of steel depends only on the concentration of carbon in steel. Therefore it may be enough to have high carbon only at the surface. This can be achieved by increasing the concentration of carbon in a component made of low carbon steel by allowing carbon to diffuse into it. The rate at which carbon can diffuse depends on its concentration gradient and its diffusivity in steel. A high concentration gradient can be maintained only if there is a significant difference in the concentration of carbon at the surface and the core. A high temperature would certainly ensure high diffusivity. One of the ways to achieve this is to heat low carbon steel (< 0.2%C) kept in a packed bed to around 1000°C. The process is known as pack carburizing. The basic principles of the process have been explained with the help of a few diagrams in slide 4. The sketch (a) shows what would be best temperature for carburization. There are
two dotted horizontal lines on the same sketch. These are labeled as T1 and T2. Note that %C in steel is
C0. At room temperature its microstructure consists of ferrite and pearlite. When it is heated to T1 pearlite transforms into austenite. The sample now consists of ferrite and austenite. Out of the two the ferrite is saturated with carbon. It is impossible to maintain any concentration gradient between its surface and its centre. However the austenite in low carbon steel at this temperature is not saturated
with carbon. C1 denotes the likely difference in %C that can be maintained at T1. The microstructure of
low carbon steel at T2 is 100%austenite. The solubility limit of carbon in austenite is much higher than
C0. C2 denotes the likely difference in %C that can be maintained at T2. C2 is much greater than C1.
Therefore selection of T2 as the carburization temperature is more appropriate.
Pack carburizing: LC steel
(a) (b) C2 Sample T2 A3 C1 T1 T A1 + cm 85% char coal + 15% energizer C0 %C CS BaCO3 = BaO + CO2 Slide 4 (c) C S CO2 + C = 2 CO (d) C 0 2 CO = C (Fe) + CO % t 2 C CS : Function ( Temp) x 9 Depth: F (T,t)
NPTEL Phase II : IIT Kharagpur : Prof. R. N. Ghosh, Dept of Metallurgical and Materials Engineering || | |
The sketch (b) in slide 4 shows a schematic representation of how the sample is placed within a mixture
of BaCO3 (energizer) and char coal. At 1000°C, the carburization temperature, BaCO3 decomposes to
give CO2. In the presence of excess carbon CO2 is converted into CO which later decomposes in the presence of Fe leaving a film of nascent carbon on the surface of the steel component. This
reacts with Fe in steel to form Fe3C. The concentration of carbon in austenite near the carbide
layer is given by the phase diagram. In this case it is CS. It is a function of temperature. The sketch (c) gives a schematic map showing carbon concentration gradient. The sketch (d) gives
the expected concentration versus distance (x: from the surface to the centre) plots at T2. It is a function of both temperature (T) and time (t).
Carburization depth (a) CC x 0 erf CC CS C0 S 0 2 Dt x Q C DDC 0 exp S RT erf (0.5) 0.5 C0 Slide 5 xDt (b) d x
-4 Problem: T=927 C, t=10hrs, C0=0.2, D0= 0.7x10 2 m /s Q=157 kJ/mole, CS=1.2 Estimate x. erf(z) = z
Slide 5 describes a method of estimating the concentration of carbon in a steel specimen as function of distance from its surface. At the carburization temperature the concentration of
carbon at the surface is maintained at CS whereas far away from the surface it is C0. It can therefore be visualized as a semi‐infinite diffusion couple as shown in sketch (a). The concentration profile at any instant may be described by Fick’s second law of diffusion as shown in equation 1.