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Corrosion-resistant Alloys

aluminium bronzeCorrosion-resistant alloys, as their name indicates, are alloys with enhanced corrosion resistance. Some ferrous and many non-ferrous metals and alloys are widely used in corrosive environments. In all cases, it strongly depends on certain environments and other conditions. Corrosion-resistant alloys are used for water piping and many chemical and industrial applications. In the case of ferrous alloys, we are talking about stainless steel and to some extent about cast irons. But some non-ferrous corrosion-resistant alloys exhibit remarkable corrosion resistance; therefore, they may be used for many special purposes. There are two main reasons why non-ferrous materials are preferred over steel and stainless steel for many applications. For example, many non-ferrous metals and alloys possess much higher resistance to corrosion than available alloy steels and stainless steel grades. Second, a high strength-to-weight ratio or high thermal and electrical conductivity may provide a distinct advantage over a ferrous alloy.

corrosion-resistant alloys - composition

Types of Corrosion-resistant Alloys

Four common non-ferrous metals used for their well-documented corrosion resistance properties are:

  • Nibral Propeller (nickel aluminium bronze) Source: generalpropeller.com
    Nibral Propeller (nickel aluminium bronze) Source: generalpropeller.com

    Copper. Copper does not react with water, but it slowly reacts with atmospheric oxygen to form a layer of brown-black copper oxide which, unlike the rust that forms on iron in moist air, protects the underlying metal from further corrosion (passivation). Copper-nickel alloys and aluminium bronze demonstrate superior resistance to saltwater corrosion. For example, cupronickels are copper-nickel alloys that typically contain 60 to 90 percent copper and nickel as the main alloying element. The two main alloys are 90/10 and 70/30. Other strengthening elements, such as manganese and iron, may also be contained. Cupronickels have excellent resistance to corrosion caused by seawater. Despite its high copper content, cupronickel is silver in color. Adding nickel to copper improves strength and corrosion resistance, but good ductility is retained. Cupronickels may be used in many marine applications, such as for propellers and propeller shafts. Since cupronickel alloys have an inherent resistance to macrofouling, good tensile strength, excellent ductility when annealed, high thermal conductivity, and expansion characteristics, they may be used for heat exchangers, such as in steam turbine condensers, oil coolers, auxiliary cooling systems, and high-pressure pre-heaters at nuclear and fossil fuel power plants. Another very common corrosion-resistant material is aluminium bronze, which has excellent corrosion resistance, especially in seawater and similar environments, where the alloys often outperform many stainless steels. Their excellent resistance to corrosion results from the aluminium in the alloys, which reacts with atmospheric oxygen to form a thin, tough surface layer of alumina (aluminium oxide) which acts as a barrier to corrosion of the copper-rich alloy. They are found in wrought and cast form. Aluminium bronzes are usually golden in color. Aluminium bronzes are used in seawater applications that include:

    • General sea water-related services
    • Bearings
    • Pipe fittings
    • Pumps and valve components
    • Heat exchangers
  • superalloys - inconel - turbine bladeNickel. Nickel is a silvery-white lustrous metal with a slight golden tinge. Nickel is one of the most common alloying elements. About 65% of nickel production is used in stainless steel. Because nickel does not form any carbide compounds in steel, it remains in solution in the ferrite, thus strengthening and toughening the ferrite phase. Nickel steels are easily heat treated because nickel lowers the critical cooling rate. Nickel-based alloys (e.g., Fe-Cr-Ni(Mo) alloys) exhibit excellent ductility and toughness, even at high strength levels and these properties are retained up to low temperatures. Nickel and its alloys are highly resistant to corrosion in many environments, especially basic (alkaline). Nickel also reduces thermal expansion for better dimensional stability. Nickel is the base element for superalloys. These metals have excellent resistance to thermal creep deformation and retain their stiffness, strength, toughness, and dimensional stability at temperatures much higher than the other aerospace structural materials. For example, Inconel is a registered trademark of Special Metals for a family of austenitic nickel-chromium-based superalloys. Inconel 718 is a nickel-based superalloy with high strength properties and resistance to elevated temperatures. It also demonstrates remarkable protection against corrosion and oxidation. They were initially developed for use in aircraft piston engine turbosuperchargers. Today, the most common application is in aircraft turbine components, which must withstand exposure to severely oxidizing environments and high temperatures for reasonable periods.
  • Titanium. Pure titanium is stronger than common, low-carbon steels but 45% lighter. It is also twice as strong as weak aluminium alloys but only 60% heavier. The two most useful properties of the metal are corrosion resistance and strength-to-density ratio, the highest of any metallic element. The corrosion resistance of titanium alloys at normal temperatures is unusually high. Titanium’s corrosion resistance is based on forming a stable, protective oxide layer. Although “commercially pure” titanium has acceptable mechanical properties and has been used for orthopedic and dental implants, for most applications titanium is alloyed with small amounts of aluminium and vanadium, typically 6% and 4% respectively, by weight. This mixture has a solid solubility that varies dramatically with temperature, allowing it to undergo precipitation strengthening. Titanium alloys are metals that contain a mixture of titanium and other chemical elements. Such alloys have high tensile strength and toughness (even at extreme temperatures). They are light in weight, have extraordinary corrosion resistance, and can withstand extreme temperatures. For example, commercially pure titanium grade 2 is very similar to grade 1, but it has higher strength than grade 1 and excellent cold forming properties. It provides excellent welding properties and has excellent resistance to oxidation and corrosion. This titanium grade is the most common in the commercially pure titanium industry. It is the prime choice for many fields of applications:
    • Aerospace,
    • Automotive,
    • Chemical Processing & Chlorate Manufacturing,
    • Desalination
    • Power generation
  • Aluminium. In general, aluminium alloys are characterized by a relatively low density (2.7 g/cm3 compared to 7.9 g/cm3 for steel), high electrical and thermal conductivities, and resistance to corrosion in some common environments, including the ambient atmosphere. Its corrosion resistance strongly depends on certain alloys. For example, duralumin is due to the presence of copper susceptible to corrosion, while 6061 alloy remains resistant to corrosion even when the surface is abraded. At higher temperatures and in aggressive environments, aluminium alloys have poor corrosion resistance and suffer from stress corrosion cracking.

Stainless Steels – Ferrous Corrosion-resistant Alloys

Although we are discussing primarily non-ferrous corrosion-resistant alloys, we must mention stainless steel. Stainless steels are defined as low-carbon steels with at least 10.5% chromium with or without other alloying elements and a maximum of 1.2% carbon by mass. Stainless steels, also known as inox steels or inox from French inoxydable (inoxidizable), are steel alloys that are very well known for their corrosion resistance, which increases with increasing chromium content. Corrosion resistance may also be enhanced by nickel and molybdenum additions.

stainless steel - tubeAustenitic stainless steels have the best corrosion resistance of all stainless steels, and they have excellent cryogenic properties and good high-temperature strength. They possess a face-centered cubic (fcc) microstructure that is nonmagnetic and can be easily welded. This austenite crystalline structure is achieved by sufficient additions of the austenite stabilizing elements nickel, manganese, and nitrogen. Austenitic stainless steel is the largest family of stainless steel, making up two-thirds of all stainless steel production.

The resistance of these metallic alloys to the chemical effects of corrosive agents is based on passivation. For passivation to occur and remain stable, the Fe-Cr alloy must have a minimum chromium content of about 10.5% by weight, above which passivity can occur and below is impossible. The strength and corrosion resistance of stainless steel often make it the material of choice in transportation and processing equipment, engine parts, and firearms. Most structural applications occur in the chemical and power engineering industries, which account for more than a third of the market for stainless steel products. The wide variety of applications includes nuclear reactor vessels and heat exchangers.

Stress-corrosion cracking

One of the most serious metallurgical problems and a major concern in the nuclear industry is stress-corrosion cracking (SCC). Stress-corrosion cracking results from the combined action of applied tensile stress and a corrosive environment, and both influences are necessary. SCC is a type of intergranular attack corrosion that occurs at the grain boundaries under tensile stress. Low alloy steels are less susceptible than high alloy steels but are subject to SCC in water containing chloride ions. Nickel-based alloys, however, are not effected by chloride or hydroxide ions. An example of a nickel-based alloy resistant to stress-corrosion cracking is Inconel.

Properties of Corrosion-resistant Alloys

Material properties are intensive properties, which means they are independent of the amount of mass and may vary from place to place within the system at any moment. Materials science involves studying materials’ structure and relating them to their properties (mechanical, electrical, etc.). Once materials scientist knows about this structure-property correlation, they can then go on to study the relative performance of a material in a given application. The major determinants of the structure of a material and, thus, its properties are its constituent chemical elements and the way it has been processed into its final form.

The density of Corrosion-resistant Alloys

The density of a typical aluminium bronze is 7.45 g/cm3 (UNS C95400).

The density of a typical superalloy is 8.22 g/cm3 (Inconel 718).

The density of a typical titanium alloy is 4.51 g/cm3 (Grade 2).

The density of a typical aluminium alloy is 2.7 g/cm3 (6061 alloys).

The density of typical stainless steel is 8.0 g/cm3 (304 steel).

Density is defined as the mass per unit volume. It is an intensive property, which is mathematically defined as mass divided by volume:

ρ = m/V

In words, the density (ρ) of a substance is the total mass (m) of that substance divided by the total volume (V) occupied by that substance. The standard SI unit is kilograms per cubic meter (kg/m3). The Standard English unit is pounds mass per cubic foot (lbm/ft3).

Since the density (ρ) of a substance is the total mass (m) of that substance divided by the total volume (V) occupied by that substance, it is obvious that the density of a substance strongly depends on its atomic mass and also on the atomic number density (N; atoms/cm3),

  • Atomic Weight. The atomic mass is carried by the atomic nucleus, which occupies only about 10-12 of the atom’s total volume or less, but it contains all the positive charge and at least 99.95% of the atom’s total mass. Therefore it is determined by the mass number (number of protons and neutrons).
  • Atomic Number Density. The atomic number density (N; atoms/cm3), which is associated with atomic radii, is the number of atoms of a given type per unit volume (V; cm3) of the material. The atomic number density (N; atoms/cm3) of a pure material having an atomic or molecular weight (M; grams/mol) and the material density (⍴; gram/cm3) is easily computed from the following equation using Avogadro’s number (NA = 6.022×1023 atoms or molecules per mole):Atomic Number Density
  • Crystal Structure. The density of a crystalline substance is significantly affected by its crystal structure. FCC structure, along with its hexagonal relative (hcp), has the most efficient packing factor (74%). Metals containing FCC structures include austenite, aluminum, copper, lead, silver, gold, nickel, platinum, and thorium.

Mechanical Properties of Corrosion-resistant Alloys

Materials are frequently chosen for various applications because they have desirable combinations of mechanical characteristics. For structural applications, material properties are crucial, and engineers must consider them.

Strength of Corrosion-resistant Alloys

In the mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. The strength of materials considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. The strength of a material is its ability to withstand this applied load without failure or plastic deformation.

Ultimate Tensile Strength

The ultimate tensile strength of aluminium bronze – UNS C95400 is about 550 MPa.

The ultimate tensile strength of superalloy – Inconel 718 depends on the heat treatment process, but it is about 1200 MPa.

The ultimate tensile strength of commercially pure titanium – Grade 2 is about 340 MPa.

The ultimate tensile strength of 6061 aluminium alloy depends greatly on the temper of the material, but for T6 temper it is about 290 MPa.

The ultimate tensile strength of stainless steel – type 304 is 515 MPa.

Yield Strength - Ultimate Tensile Strength - Table of MaterialsThe ultimate tensile strength is the maximum on the engineering stress-strain curve. This corresponds to the maximum stress that a structure in tension can sustain. Ultimate tensile strength is often shortened to “tensile strength” or “the ultimate.” If this stress is applied and maintained, a fracture will result. Often, this value is significantly more than the yield stress (as much as 50 to 60 percent more than the yield for some types of metals). When a ductile material reaches its ultimate strength, it experiences necking where the cross-sectional area reduces locally. The stress-strain curve contains no higher stress than the ultimate strength. Even though deformations can continue to increase, the stress usually decreases after achieving the ultimate strength. It is an intensive property; therefore its value does not depend on the size of the test specimen. However, it depends on other factors, such as the specimen preparation, the presence or otherwise of surface defects, and the temperature of the test environment and material. Ultimate tensile strengths vary from 50 MPa for aluminum to as high as 3000 MPa for very high-strength steels.

Yield Strength

The yield strength of aluminium bronze – UNS C95400 is about 250 MPa.

The yield strength of superalloy – Inconel 718 depends on the heat treatment process, but it is about 1030 MPa.

The yield strength of commercially pure titanium – Grade 2 is about 300 MPa.

The yield strength of 6061 aluminium alloy depends greatly on the temper of the material, but for T6 temper it is about 240 MPa.

The yield strength of stainless steel – type 304 is  205 MPa.

The yield point is the point on a stress-strain curve that indicates the limit of elastic behavior and the beginning plastic behavior. Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically. In contrast, the yield point is where nonlinear (elastic + plastic) deformation begins. Before the yield point, the material will deform elastically and return to its original shape when the applied stress is removed. Once the yield point is passed, some fraction of the deformation will be permanent and non-reversible. Some steels and other materials exhibit a behavior termed a yield point phenomenon. Yield strengths vary from 35 MPa for low-strength aluminum to greater than 1400 MPa for high-strength steel.

Young’s Modulus of Elasticity

Young’s modulus of elasticity of aluminium bronze – UNS C95400 is about 110 GPa.

Young’s modulus of elasticity of superalloy – Inconel 718 is 200 GPa.

Young’s modulus of elasticity of commercially pure titanium – Grade 2 is about 105 GPa.

Young’s modulus of elasticity of 6061 aluminium alloy is about 69 GPa.

Young’s modulus of elasticity stainless steel – type 304 and 304L is 193 GPa.

Young’s modulus of elasticity is the elastic modulus for tensile and compressive stress in the linear elasticity regime of a uniaxial deformation and is usually assessed by tensile tests. Up to limiting stress, a body will be able to recover its dimensions on the removal of the load. The applied stresses cause the atoms in a crystal to move from their equilibrium position, and all the atoms are displaced the same amount and still maintain their relative geometry. When the stresses are removed, all the atoms return to their original positions, and no permanent deformation occurs. According to Hooke’s law, the stress is proportional to the strain (in the elastic region), and the slope is Young’s modulus. Young’s modulus is equal to the longitudinal stress divided by the strain.

The hardness of Corrosion-resistant Alloys

Brinell hardness of aluminium bronze – UNS C95400 is approximately 170 MPa.

Brinell hardness of superalloy – Inconel 718 depends on the heat treatment process, but it is approximately 330 MPa.

Rockwell hardness of commercially pure titanium – Grade 2 is approximately 80 HRB.

Brinell hardness of 6061 aluminium alloy depends greatly on the temper of the material, but for T6 temper it is approximately 95 MPa.

Brinell hardness of stainless steel – type 304 is approximately 201 MPa.

Brinell hardness number

Rockwell hardness test is one of the most common indentation hardness tests, that has been developed for hardness testing. In contrast to the Brinell test, the Rockwell tester measures the depth of penetration of an indenter under a large load (major load) compared to the penetration made by a preload (minor load). The minor load establishes the zero posi, and the major load is applied and removed while maintaining the minor load. The difference between the penetration depth before and after applying the major load is used to calculate the Rockwell hardness number. That is, the penetration depth and hardness are inversely proportional. The chief advantage of Rockwell hardness is its ability to display hardness values directly. The result is a dimensionless number noted as HRA, HRB, HRC, etc., where the last letter is the respective Rockwell scale.

The Rockwell C test is performed with a Brale penetrator (120°diamond cone) and a major load of 150kg.

Thermal Properties of Corrosion-resistant Alloys

Thermal properties of materials refer to the response of materials to changes in their temperature and to the application of heat. As a solid absorbs energy in the form of heat, its temperature rises, and its dimensions increase. But different materials react to the application of heat differently.

Heat capacity, thermal expansion, and thermal conductivity are often critical in solids’ practical use.

Melting Point of Corrosion-resistant Alloys

The melting point of aluminium bronze – UNS C95400 is around 1030°C.

The melting point of superalloy – Inconel 718 steel is around 1400°C.

The melting point of commercially pure titanium – Grade 2 is around 1660°C.

The melting point of 6061 aluminium alloy is around 600°C.

The melting point of stainless steel – type 304 steel is around 1450°C.

In general, melting is a phase change of a substance from the solid to the liquid phase. The melting point of a substance is the temperature at which this phase change occurs. The melting point also defines a condition where the solid and liquid can exist in equilibrium.

Thermal Conductivity of Corrosion-resistant Alloys

The thermal conductivity of aluminium bronze – UNS C95400 is 59 W/(m. K).

The thermal conductivity of superalloy – Inconel 718 is 6.5 W/(m. K).

The thermal conductivity of commercially pure titanium – Grade 2 is 16 W/(m. K).

The thermal conductivity of 6061 aluminium alloy is 150 W/(m. K).

The thermal conductivity of stainless steel – type 304 is 20 W/(m. K).

The heat transfer characteristics of solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It measures a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies to all matter, regardless of its state (solid, liquid, or gas), therefore, it is also defined for liquids and gases.

The thermal conductivity of most liquids and solids varies with temperature, and for vapors, it also depends upon pressure. In general:

thermal conductivity - definition

Most materials are nearly homogeneous, therefore, we can usually write k = k (T). Similar definitions are associated with thermal conductivities in the y- and z-directions (ky, kz), but for an isotropic material the thermal conductivity is independent of the direction of transfer, kx = ky = kz = k.

References:
Materials Science:

U.S. Department of Energy, Material Science. DOE Fundamentals Handbook, Volume 1 and 2. January 1993.
U.S. Department of Energy, Material Science. DOE Fundamentals Handbook, Volume 2 and 2. January 1993.
William D. Callister, David G. Rethwisch. Materials Science and Engineering: An Introduction 9th Edition, Wiley; 9 edition (December 4, 2013), ISBN-13: 978-1118324578.
Eberhart, Mark (2003). Why Things Break: Understanding the World, by the Way, It Comes Apart. Harmony. ISBN 978-1-4000-4760-4.
Gaskell, David R. (1995). Introduction to the Thermodynamics of Materials (4th ed.). Taylor and Francis Publishing. ISBN 978-1-56032-992-3.
González-Viñas, W. & Mancini, H.L. (2004). An Introduction to Materials Science. Princeton University Press. ISBN 978-0-691-07097-1.
Ashby, Michael; Hugh Shercliff; David Cebon (2007). Materials: engineering, science, processing, and design (1st ed.). Butterworth-Heinemann. ISBN 978-0-7506-8391-3.
J. R. Lamarsh, A. J. Baratta, Introduction to Nuclear Engineering, 3d ed., Prentice-Hall, 2001, ISBN: 0-201-82498-1.

See above:
Alloys