Steel’s properties
The primary ingredient in the steel are iron. Iron is a metallic that , when it is in its natural state is not as hard as copper. Omitting very extreme cases, iron in its solid state is, like all other metals, polycrystalline–that is, it consists of many crystals that join one another on their boundaries. Crystals are a well-organized arrangement of atoms, which could be best described as spheres that are touching each other. They are organized by lattices or planes that are able to penetrate each other in particular ways. Iron’s arrangement of lattices is best visualized using an unicube that has eight iron atoms in its corners. One of the most significant aspects that distinguish steel is the iron’s allotropy, that is, it exists in two crystal forms.
For the body-centred cubic (bcc) arrangement there is an extra iron atom located in the middle of every cube. When you look at the faces-centred cubic (fcc) arrangement there is an additional iron atom in the middle on each face of the cube. It is important to note that the faces of the face-centred cubic cube, as well as the spacing between adjacent lattices of the fcc arrangement approximately 25 percent more than the bcc configuration. This implies the fcc has more space within the fcc structure than in the BCC structure, which is designed to prevent alien ( i.e., alloying) elements from forming alloys within solid
The effects on carbon
In its natural form iron is a soft material and is generally ineffective for engineering purposes; the primary method for strengthening it and turning the material into steel comes adding tiny quantities of carbon. In steel that is solid, carbon is typically present as two different forms. It can be found in the form of a solid solution, such as austenite and ferrite or as a carbonate. The carbide form could include iron carbonate (Fe 3C, also known in the form of cementite) or it could be a carbide from an alloying element like  (On the contrary in gray iron, carbon is seen as crystals or flakes made of graphite due to the fact that there is silicon that blocks the formation of carbide.)
The carbon effects can be best illustrated using the iron carbon equilibrium diagram. The A-B-C line is a representation of Liquius Points ( i.e., the temperature at which iron melts begin to begin to solidify) and the H-J E-C line indicates the points of solidus (at when solidification is complete). The A-B C line shows that temperatures for solidification decrease because the carbon content in an iron melt increases. (This is the reason the reason why gray iron, with greater than two percent carbon is processed at lesser temperatures than iron.) Molten steel that has an example of this, for instance, the carbon percentage that is 0.77 percent (shown by the vertical dashed line in this figure) starts to form solid around 1,475deg C (2,660deg F) and then becomes fully solid around 1400deg C (2,550deg Fahrenheit). From this point on the iron crystals remain in an austenitic state.
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arrangement
and include all the carbon present in and around the carbon in solid solution. As the solution cools and a drastic change is observed at 727deg C (1,341deg F) when the austenite crystals change into a fine, lamellar structure comprised of alternating plates composed of iron carbide and ferrite. The microstructure is referred to as pearlite and the process is known as the eutectoidic change. Pearlite is a diamond-like pyramid with a hardness (DPH) that is approximately 200 kilograms of force for each square millimeter (285,000 pounds/square inch) as compared to the DPH of 70 kilograms-force for each square millimetre of pure iron. The cooling of steel with less carbon ( e.g., 0.25 percent) creates an atomic structure that is comprised of 50 percent pearlite and 50 percent ferrrite which is less hard than pearlite and has an DPH of approximately 130. Steel that has more thanÂ
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