Alloying a metal is done by combining it with one or more other elements. The most common and oldest alloying process is performed by heating the base metal beyond its
melting point and then dissolving the solutes into the molten liquid, which may be possible even if the melting point of the solute is far greater than that of the base. For example, in its liquid state, titanium is a very strong solvent capable of dissolving most metals and elements. In addition, it readily absorbs gases like oxygen and burns in the presence of nitrogen. This increases the chance of contamination from any contacting surface, and so must be melted in vacuum induction-heating and special, water-cooled, copper
crucibles. lattice Carbon has a very high melting-point and only does so under high atmospheric pressure, so it was impossible for ancient civilizations to combine with iron as a liquid solute. However, alloying (in particular, interstitial alloying) may be performed with one or more constituents in a gaseous state, such as found in a
blast furnace to make pig iron (liquid-gas),
nitriding,
carbonitriding or other forms of
case hardening (solid-gas), or the
cementation process used to make
blister steel (solid-gas). It may also be done with one, more, or all of the constituents in the solid state, such as found in ancient methods of
pattern welding (solid-solid),
shear steel (solid-solid), or
crucible steel production (solid-liquid), mixing the elements via solid-state
diffusion. By adding another element to a metal, differences in the size of the atoms create internal stresses in the lattice of the metallic crystals; stresses that often enhance its properties. For example, the combination of carbon with
wrought iron produces steel, which is stronger than iron, its primary element. The
electrical and
thermal conductivity of alloys is usually lower than that of the pure metals. The physical properties, such as
density,
reactivity,
Young's modulus of an alloy may not differ greatly from those of its base element, but engineering properties such as
tensile strength, ductility, and
shear strength may be substantially different from those of the constituent materials. This is sometimes a result of the sizes of the
atoms in the alloy, because larger atoms exert a compressive force on neighboring atoms, and smaller atoms exert a tensile force on their neighbors, helping the alloy resist deformation. Sometimes alloys may exhibit marked differences in behavior even when small amounts of one element are present. For example, impurities in semiconducting
ferromagnetic alloys lead to different properties, as first predicted by White, Hogan, Suhl, Tian Abrie and Nakamura. Unlike pure metals, most alloys do not have a single
melting point, but a melting range during which the material is a mixture of
solid and
liquid phases (a slush). The temperature at which melting begins is called the
solidus, and the temperature when melting is just complete is called the
liquidus. For many alloys there is a particular alloy proportion (in some cases more than one), called either a
eutectic mixture or a peritectic composition, which gives the alloy a unique and low melting point, and no liquid/solid slush transition.
Heat treatment , (
alpha iron and
gamma iron) showing the differences in atomic arrangement (slowly cooled) steel forms a heterogeneous, lamellar microstructure called
pearlite, consisting of the phases
cementite (light) and
ferrite (dark). Bottom photo:
Quenched (quickly cooled) steel forms a single phase called
martensite, in which the carbon remains trapped within the crystals, creating internal stresses Alloying elements are added to a base metal, to induce
hardness,
toughness, ductility, or other desired properties. Many metals and alloys can be
work hardened by creating defects in their crystal structure. These defects are created during
plastic deformation by hammering, bending, extruding, et cetera, and are permanent unless the metal is
recrystallized. Otherwise, some alloys can also have their properties altered by
heat treatment. Nearly all metals can be softened by
annealing, which recrystallizes the alloy and repairs the defects, but not as many can be hardened by controlled heating and cooling. Many alloys of aluminium, copper,
magnesium, titanium, and nickel can be strengthened to some degree by some method of heat treatment, but few respond to this to the same degree as does steel. This allows the smaller carbon atoms to enter the interstices of the iron crystal. When this
diffusion happens, the carbon atoms are said to be in
solution in the iron, forming a particular single, homogeneous, crystalline phase called
austenite. If the steel is cooled slowly, the carbon can diffuse out of the iron and it will gradually revert to its low temperature allotrope. During slow cooling, the carbon atoms will no longer be as
soluble with the iron, and will be forced to
precipitate out of solution,
nucleating into a more concentrated form of iron carbide (Fe3C) in the spaces between the pure iron crystals. The steel then becomes heterogeneous, as it is formed of two phases, the iron-carbon phase called
cementite (or
carbide), and pure iron
ferrite. Such a heat treatment produces a steel that is rather soft. If the steel is cooled quickly, however, the carbon atoms will not have time to diffuse and precipitate out as carbide, but will be trapped within the iron crystals. When rapidly cooled, a
diffusionless (martensite) transformation occurs, in which the carbon atoms become trapped in solution. This causes the iron crystals to deform as the crystal structure tries to change to its low temperature state, leaving those crystals very hard but much less ductile (more brittle). While the high strength of steel results when diffusion and precipitation is prevented (forming martensite), most heat-treatable alloys are
precipitation hardening alloys, that depend on the diffusion of alloying elements to achieve their strength. When heated to form a solution and then cooled quickly, these alloys become much softer than normal, during the diffusionless transformation, but then harden as they age. The solutes in these alloys will precipitate over time, forming
intermetallic phases, which are difficult to discern from the base metal. Unlike steel, in which the solid solution separates into different crystal phases (carbide and ferrite), precipitation hardening alloys form different phases within the same crystal. These intermetallic alloys appear homogeneous in crystal structure, but tend to behave heterogeneously, becoming hard and somewhat brittle. Wilm had been searching for a way to harden aluminium alloys for use in machine-gun cartridge cases. Knowing that aluminium-copper alloys were heat-treatable to some degree, Wilm tried quenching a ternary alloy of aluminium, copper, and the addition of magnesium, but was initially disappointed with the results. However, when Wilm retested it the next day he discovered that the alloy increased in hardness when left to age at room temperature, and far exceeded his expectations. Although an explanation for the phenomenon was not provided until 1919,
duralumin was one of the first "age hardening" alloys used, becoming the primary building material for the first
Zeppelins, and was soon followed by many others. Because they often exhibit a combination of high strength and low weight, these alloys became widely used in many forms of industry, including the construction of modern
aircraft.
Mechanisms When a molten metal is mixed with another substance, there are two mechanisms that can cause an alloy to form, called
atom exchange and the
interstitial mechanism. The relative size of each element in the mix plays a primary role in determining which mechanism will occur. When the atoms are relatively similar in size, the atom exchange method usually happens, where some of the atoms composing the metallic crystals are substituted with atoms of the other constituent. This is called a
substitutional alloy. Examples of substitutional alloys include bronze and brass, in which some of the copper atoms are substituted with either tin or zinc atoms respectively. In the case of the interstitial mechanism, one atom is usually much smaller than the other and can not successfully substitute for the other type of atom in the crystals of the base metal. Instead, the smaller atoms become trapped in the
interstitial sites between the atoms of the crystal matrix. This is referred to as an
interstitial alloy. Steel is an example of an interstitial alloy, because the very small carbon atoms fit into interstices of the iron matrix. == History and examples ==