Nick Connor

About Polystyrene

Polystyrene, abbreviated as PS, is a synthetic aromatic hydrocarbon polymer made from the monomer known as styrene, which is derived from benzene and ethylene, both petroleum products. Polystyrene can be solid or foamed. General-purpose polystyrene is clear, hard, and rather brittle. Polystyrene is a colorless, transparent thermoplastic, which is commonly used to make foam board or beadboard insulation and a type of loose-fill insulation consisting of small beads of polystyrene. Polystyrene foams are 95-98% air. Polystyrene foams are good thermal insulators and are therefore often used as building insulation materials, such as in insulating concrete forms and structural insulated panel building systems. Expanded (EPS) and extruded polystyrene (XPS) are both made from polystyrene, but EPS is composed of small plastic beads that are fused together and XPS begins as a molten material that is pressed out of a form into sheets. XPS is most commonly used as foam board insulation.

Summary

Name	Polystyrene
Phase at STP	solid
Density	1050 kg/m3
Ultimate Tensile Strength	48 MPa
Yield Strength	N/A
Young’s Modulus of Elasticity	3.4 GPa
Brinell Hardness	50 BHN
Melting Point	217 °C
Thermal Conductivity	0.12 W/mK
Heat Capacity	1100 J/g K
Price	1.1 $/kg

Composition of Polystyrene

In chemical terms, polystyrene is a long chain hydrocarbon wherein alternating carbon centers are attached to phenyl groups (a derivative of benzene). Polystyrene’s chemical formula is (C8H8)n; it contains the chemical elements carbon and hydrogen.

Applications of Polystyrene

PS is one of the four plastics whose combined usage accounts for 75 percent of the worldwide usage of plastics. These four commodity thermoplastics are PE, PP, PVC, and PS. Applications include toys, light diffusers, beakers, cutlery, general household appliances, video/audio cassette cases, electronic housings, refrigerator liners, housewares, containers.

Mechanical Properties of Polystyrene

Strength of Polystyrene

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of Polystyrene

Ultimate tensile strength of Polystyrene is 48 MPa.

Yield Strength of Polystyrene

Yield strength of Polystyrene is N/A.

Modulus of Elasticity of Polystyrene

The Young’s modulus of elasticity of Polystyrene is 3.4 GPa.

Hardness of Polystyrene

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Brinell hardness of Polystyrene is approximately 50 BHN (converted).

See also: Hardness of Materials

Thermal Properties of Polystyrene

Polystyrene – Melting Point

Melting point of Polystyrene is 217 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Polystyrene – Thermal Conductivity

Thermal conductivity of Polystyrene is 0.12 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Polystyrene – Specific Heat

Specific heat of Polystyrene is 1100 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About Uranium Dioxide

Uranium dioxide is a ceramic refractory uranium compound, in many cases used as a nuclear fuel. Most of LWRs use the uranium fuel, which is in the form of uranium dioxide (chemically UO2). Uranium dioxide is a black semiconducting solid with very low thermal conductivity. On the other hand the uranium dioxide has very high melting point and has well known behavior. Uranium dioxide has significantly lower density than uranium in the metal form. Uranium dioxide has a density of 10.97 g/cm3, but this value may vary with fuel burnup, because at low burnup densification of pellets can occurs and at higher burnup swelling occurs.

Summary

Name	Uranium Dioxide
Phase at STP	solid
Density	10970 kg/m3
Ultimate Tensile Strength	N/A
Yield Strength	N/A
Young’s Modulus of Elasticity	N/A
Brinell Hardness	N/A
Melting Point	2847 °C
Thermal Conductivity	8.68 W/mK
Heat Capacity	235 J/g K
Price	60 $/kg

Composition of Uranium Dioxide

The UO2 is pressed into pellets, these pellets are then sintered into the solid cylinder (with a height, and diameter of about 1 centimeter, the height being greater than the diameter).

Applications of Uranium Dioxide

Most of PWRs use the uranium fuel, which is in the form of uranium dioxide.

Thermal Properties of Uranium Dioxide

Uranium Dioxide – Melting Point

Melting point of Uranium Dioxide is 2847 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Uranium Dioxide – Thermal Conductivity

Thermal conductivity of Uranium Dioxide is 8.68 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Uranium Dioxide – Specific Heat

Specific heat of Uranium Dioxide is 235 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About Ruby

A ruby is a pink to blood-red coloured gemstone, a variety of the mineral corundum (aluminium oxide). Other varieties of gem-quality corundum are called sapphires. Rubies have a hardness of 9.0 on the Mohs scale of mineral hardness.

Summary

Name	Ruby
Phase at STP	solid
Density	3980 kg/m3
Ultimate Tensile Strength	2100 MPa
Yield Strength	N/A
Young’s Modulus of Elasticity	350 GPa
Brinell Hardness	9 Mohs
Melting Point	2047 °C
Thermal Conductivity	40 W/mK
Heat Capacity	750 J/g K
Price	50000000 $/kg

Composition of Ruby

Sapphire, ruby, and pure corundum are α-alumina, the most stable form of Al2O3.

Applications of Ruby

Like other gemstones, rubies are becoming an increasingly popular choice for engagement rings and other jewelry.

Mechanical Properties of Ruby

Strength of Ruby

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of Ruby

Ultimate tensile strength of Ruby is 2100 MPa (compressive).

Yield Strength of Ruby

Yield strength of Ruby is N/A.

Modulus of Elasticity of Ruby

The Young’s modulus of elasticity of Ruby is 350 GPa.

Hardness of Ruby

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Hardness of Ruby is approximately 9 Mohs.

See also: Hardness of Materials

Thermal Properties of Ruby

Ruby – Melting Point

Melting point of Ruby is 2047 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Ruby – Thermal Conductivity

Thermal conductivity of Ruby is 40 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Ruby – Specific Heat

Specific heat of Ruby is 750 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About TZM Alloy

Molybdenum-titanium-zirconium (TZM) alloys contain small amounts of titanium and zirconium doped with small amounts of very fine carbides. This alloy belongs to refractory alloys, which are well known for their extraordinary resistance to heat and wear. Key requirement to withstand high temperatures is a high melting point and stable mechanical properties (e.g. high hardness) even at high temperatures. This alloy functions most efficiently in temperature ranges of 700-1400°C. The alloy exhibits a higher creep resistance and strength at high temperatures, making service temperatures of above 1060 °C possible for the material. It is typically manufactured by powder metallurgy or arc-casting processes.

Summary

Name	TZM Alloy
Phase at STP	solid
Density	10220 kg/m3
Ultimate Tensile Strength	800 MPa
Yield Strength	N/A
Young’s Modulus of Elasticity	320 GPa
Brinell Hardness	220 BHN
Melting Point	2597 °C
Thermal Conductivity	126 W/mK
Heat Capacity	305 J/g K
Price	100 $/kg

Composition of TZM Alloy

TZM alloys are molybdenum-titanium-zirconium alloys and contain small amounts of titanium and zirconium doped with small amounts of very fine carbides.

Applications of TZM Alloy

TZM alloys are used in virtually all major industries, where high temperature applications with heavy mechanical load is required. For example, aerospace, automotive, chemicals, mining, nuclear technology and metal processing.

Mechanical Properties of TZM Alloy

Strength of TZM Alloy

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of TZM Alloy

Ultimate tensile strength of TZM Alloy is 800 MPa.

Yield Strength of TZM Alloy

Yield strength of TZM Alloy is N/A.

Modulus of Elasticity of TZM Alloy

The Young’s modulus of elasticity of TZM Alloy is 320 GPa.

Hardness of TZM Alloy

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Brinell hardness of TZM Alloy is approximately 220 BHN (converted).

See also: Hardness of Materials

Thermal Properties of TZM Alloy

TZM Alloy – Melting Point

Melting point of TZM Alloy is 2597 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

TZM Alloy – Thermal Conductivity

Thermal conductivity of TZM Alloy is 126 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

TZM Alloy – Specific Heat

Specific heat of TZM Alloy is 305 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About Limestone

Limestone is very common in architecture, especially in Europe and North America. Limestone is extracted from quarries or mines. Part of the extracted stone, selected according to its chemical composition and optical granulometry, is calcinated at about 1,000 °C (1,830 °F) in different types of lime kilns to produce quicklime. The principal users of lime are steelmaking industry (lowering slag melting temperature) ~ 35 %, environmental uses (desulfurization, water cleaning) ~ 20 %, civil engineering ~ 20 % and chemistry ~ 8 %.

Summary

Name	Limestone
Phase at STP	solid
Density	2750 kg/m3
Ultimate Tensile Strength	2.5 MPa
Yield Strength	N/A
Young’s Modulus of Elasticity	34 GPa
Brinell Hardness	4 Mohs
Melting Point	1337 °C
Thermal Conductivity	1.3 W/mK
Heat Capacity	840 J/g K
Price	3 $/kg

Composition of Limestone

The main component of limestone is calcium carbonate (CaCO3), also known as calcite, which is formed by the compaction of the remains of coral animals and plants on the bottoms of oceans. It varies from a soft white substance (chalk) to a very hard substance (marble).

Applications of Limestone

Limestone is very common in architecture, especially in Europe and North America. Limestone is extracted from quarries or mines. Part of the extracted stone, selected according to its chemical composition and optical granulometry, is calcinated at about 1,000 °C (1,830 °F) in different types of lime kilns to produce quicklime. The principal users of lime are steelmaking industry (lowering slag melting temperature) ~ 35 %, environmental uses (desulfurization, water cleaning) ~ 20 %, civil engineering ~ 20 % and chemistry ~ 8 %.

Mechanical Properties of Limestone

Strength of Limestone

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of Limestone

Ultimate tensile strength of Limestone is 2.5 MPa.

Yield Strength of Limestone

Yield strength of Limestone is N/A.

Modulus of Elasticity of Limestone

The Young’s modulus of elasticity of Limestone is 34 GPa.

Hardness of Limestone

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Hardness of Limestone is approximately 4 Mohs.

See also: Hardness of Materials

Thermal Properties of Limestone

Limestone – Melting Point

Melting point of Limestone is 1337 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Limestone – Thermal Conductivity

Thermal conductivity of Limestone is 1.3 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Limestone – Specific Heat

Specific heat of Limestone is 840 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About Sand

Sand is a granular material composed of finely divided rock and mineral particles. The composition of sand varies, depending on the local rock sources and conditions, but the most common constituent of sand in inland continental settings and non-tropical coastal settings is silica (silicon dioxide, or SiO2), usually in the form of quartz. Silica is one of the most complex and most abundant families of materials, existing as a compound of several minerals and as synthetic product.

Summary

Name	Sand
Phase at STP	solid
Density	1500 kg/m3
Ultimate Tensile Strength	N/A
Yield Strength	N/A
Young’s Modulus of Elasticity	N/A
Brinell Hardness	N/A
Melting Point	1577 °C
Thermal Conductivity	0.25 W/mK
Heat Capacity	830 J/g K
Price	0.03 $/kg

Composition of Sand

The composition of sand varies, depending on the local rock sources and conditions, but the most common constituent of sand in inland continental settings and non-tropical coastal settings is silica (silicon dioxide, or SiO2), usually in the form of quartz. The second most common type of sand is calcium carbonate, for example, aragonite, which has mostly been created, over the past half billion years, by various forms of life, like coral and shellfish.

Applications of Sand

Sand is a non-renewable resource over human timescales, and sand suitable for making concrete is in high demand. Because of the growth of population and of cities and the consequent construction activity there is a huge demand for these special kinds of sand, and natural sources are running low. In the pottery and glassmaking industries very pure quartzose sands are used as a source of silica. Similar sands are required for lining the hearths of acid-steel furnaces.

Mechanical Properties of Sand

Strength of Sand

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of Sand

Ultimate tensile strength of Sand is N/A.

Yield Strength of Sand

Yield strength of Sand is N/A.

Modulus of Elasticity of Sand

The Young’s modulus of elasticity of Sand is N/A.

Hardness of Sand

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Brinell hardness of Sand is approximately N/A.

See also: Hardness of Materials

Thermal Properties of Sand

Sand – Melting Point

Melting point of Sand is 1577 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Sand – Thermal Conductivity

Thermal conductivity of Sand is 0.25 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Sand – Specific Heat

Specific heat of Sand is 830 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About Carbon Monoxide

Carbon monoxide, (CO), a highly toxic, colourless, odourless, flammable gas produced industrially for use in the manufacture of numerous organic and inorganic chemical products. Carbon monoxide is not found in the air under ordinary conditions, since it is formed by incomplete carbon combustion of coal, natural gas, oil.

Summary

Name	Carbon Monoxide
Phase at STP	gas
Density	1.14 kg/m3
Ultimate Tensile Strength	N/A
Yield Strength	N/A
Young’s Modulus of Elasticity	N/A
Brinell Hardness	N/A
Melting Point	-205 °C
Thermal Conductivity	0.024 W/mK
Heat Capacity	1040 J/g K
Price	15 $/kg

Composition of Carbon Monoxide

Carbon monoxide consists of one carbon atom and one oxygen atom, connected by a triple bond that consists of a net two pi bonds and one sigma bond. It is the simplest oxocarbon and is isoelectronic with other triply-bonded diatomic species possessing 10 valence electrons.

Applications of Carbon Monoxide

Packaged carbon monoxide is used in a variety of industries for a wide range of applications including: Metal Fabrication: Used in fuel gas mixtures with hydrogen and other gases for industrial and domestic heating. Chemicals: In the manufacture of a variety of chemicals such as acids, esters and alcohols.

Thermal Properties of Carbon Monoxide

Carbon Monoxide – Melting Point

Melting point of Carbon Monoxide is -205 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Carbon Monoxide – Thermal Conductivity

Thermal conductivity of Carbon Monoxide is 0.024 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Carbon Monoxide – Specific Heat

Specific heat of Carbon Monoxide is 1040 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About Polycarbonate

Polycarbonate (PC) is a thermoplastic polymer that contains carbonate groups in its chemical structures. It is a crystal clear and colourless, amorphous engineering thermoplastic notable for its high impact resistance (which remains high down to –40°C). A disadvantage includes the need for drying and elevated-temperature processing. PC has limited chemical resistance to numerous aromatic solvents, including benzene, toluene, and xylene and has a weakness to notches.

Summary

Name	Polycarbonate
Phase at STP	solid
Density	1200 kg/m3
Ultimate Tensile Strength	60 MPa
Yield Strength	N/A
Young’s Modulus of Elasticity	2.3 GPa
Brinell Hardness	80 BHN
Melting Point	297 °C
Thermal Conductivity	0.2 W/mK
Heat Capacity	1200 J/g K
Price	2.2 $/kg

Composition of Polycarbonate

Polycarbonate (PC) is a thermoplastic polymer that contains carbonate groups in its chemical structures. A carbonate ester is an ester of carbonic acid.The structure of PC, with its carbonate and bisphenolic structures, has many characteristics that promote its distinguished properties. The rigidity of the molecule accounts for strong mechanical properties, elevated heat deflection temperatures, and high dimensional stability at elevated temperatures.

Applications of Polycarbonate

Polycarbonate is mainly used for electronic applications that capitalize on its collective safety features. Being a good electrical insulator and having heat-resistant and flame-retardant properties, it is used in various products associated with electrical and telecommunications hardware. A major application of polycarbonate is the production of Compact Discs, DVDs, and Blu-ray Discs. Applications where PC is blended with ABS increase the heat distortion temperature of the ABS and improve the low-temperature impact strength of PC. The favorable ease of processing and improved economics make PC/ABS blends well suited for thin-walled electronic housing applications such as laptop computers. PC alone is widely used as vacuum cleaner housings, household appliance housings, and power tools. These are applications where PC’s high impact strength, heat resistance, durability, and high-quality finish justify its expense. It is also used in safety helmets, riot shields, aircraft canopies, traffic light lens housings, and automotive battery cases.

Mechanical Properties of Polycarbonate

Strength of Polycarbonate

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of Polycarbonate

Ultimate tensile strength of Polycarbonate is 60 MPa.

Yield Strength of Polycarbonate

Yield strength of Polycarbonate is N/A.

Modulus of Elasticity of Polycarbonate

The Young’s modulus of elasticity of Polycarbonate is 2.3 GPa.

Hardness of Polycarbonate

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Brinell hardness of Polycarbonate is approximately 80 BHN (converted).

See also: Hardness of Materials

Thermal Properties of Polycarbonate

Polycarbonate – Melting Point

Melting point of Polycarbonate is 297 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Polycarbonate – Thermal Conductivity

Thermal conductivity of Polycarbonate is 0.2 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Polycarbonate – Specific Heat

Specific heat of Polycarbonate is 1200 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About PET

Polyethylene terephthalate, commonly abbreviated PET, PETE, is the most common thermoplastic polymer resin of the polyester family and is used in fibres for clothing, containers for liquids and foods. Polyethylene terephthalate polyester is a hard, stiff, strong, dimensionally stable material that absorbs very little water.

Summary

Name	PET
Phase at STP	solid
Density	1350 kg/m3
Ultimate Tensile Strength	150 MPa
Yield Strength	40 MPa
Young’s Modulus of Elasticity	9 GPa
Brinell Hardness	20 BHN
Melting Point	267 °C
Thermal Conductivity	0.3 W/mK
Heat Capacity	1250 J/g K
Price	0.8 $/kg

Composition of PET

PET consists of polymerized units of the monomer ethylene terephthalate, with repeating (C10H8O4) units. PET is commonly recycled, and has the number “1” as its resin identification code (RIC).

Applications of PET

There are tremendous commercial applications for PET: as an injection-molding-grade material, for blow-molded bottles, and for oriented films. The majority of the world’s PET production is for synthetic fibres (in excess of 60%), with bottle production accounting for about 30% of global demand. In the context of textile applications, PET is referred to by its common name, polyester, whereas the acronym PET is generally used in relation to packaging.

Mechanical Properties of PET

Strength of PET

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of PET

Ultimate tensile strength of PET is 150 MPa.

Yield Strength of PET

Yield strength of PET is 40 MPa.

Modulus of Elasticity of PET

The Young’s modulus of elasticity of PET is 9 GPa.

Hardness of PET

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Brinell hardness of PET is approximately 20 BHN (converted).

See also: Hardness of Materials

Thermal Properties of PET

PET – Melting Point

Melting point of PET is 267 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

PET – Thermal Conductivity

Thermal conductivity of PET is 0.3 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

PET – Specific Heat

Specific heat of PET is 1250 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution

About Graphene

Graphene is an allotrope of carbon consisting of a single layer of atoms hexagonally arranged in a two-dimensional lattice. Graphene is a substance with very interesting properties. Graphene has high thermal conductivity, high electrical conductivity, high elasticity and flexibility, high hardness and strength. These properties, together with the abundance of carbon in nature, have made graphene a very studied material with great possibilities.

Summary

Name	Graphene
Phase at STP	solid
Density	2270 kg/m3
Ultimate Tensile Strength	130000 MPa
Yield Strength	N/A
Young’s Modulus of Elasticity	1000 GPa
Brinell Hardness	N/A
Melting Point	3697 °C
Thermal Conductivity	4000 W/mK
Heat Capacity	N/A
Price	100 $/kg

Composition of Graphene

Graphene is a material composed of carbon atoms grouping that are hexagonally positioned. This arrangement results in monolayers of an atom thick. Each atom in a graphene sheet is connected to its three nearest neighbors by a σ-bond, and contributes one electron to a conduction band that extends over the whole sheet.

Applications of Graphene

Graphene is a transparent and flexible conductor that holds great promise for various material/device applications, including solar cells, light-emitting diodes (LED), touch panels, and smart windows or phones. Smartphone products with graphene touch screens are already on the market. However, with existing manufacturing processes Graphene is extremely challenging to mass produce which could prove to be a limiting factor in its commercial use.

Mechanical Properties of Graphene

Strength of Graphene

In mechanics of materials, the strength of a material is its ability to withstand an applied load without failure or plastic deformation. Strength of materials basically considers the relationship between the external loads applied to a material and the resulting deformation or change in material dimensions. In designing structures and machines, it is important to consider these factors, in order that the material selected will have adequate strength to resist applied loads or forces and retain its original shape.

Strength of a material is its ability to withstand this applied load without failure or plastic deformation. For tensile stress, the capacity of a material or structure to withstand loads tending to elongate is known as ultimate tensile strength (UTS). Yield strength or yield stress is the material property defined as the stress at which a material begins to deform plastically whereas yield point is the point where nonlinear (elastic + plastic) deformation begins. In case of tensional stress of a uniform bar (stress-strain curve), the Hooke’s law describes behaviour of a bar in the elastic region. The 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.

See also: Strength of Materials

Ultimate Tensile Strength of Graphene

Ultimate tensile strength of Graphene is 130000 MPa.

Yield Strength of Graphene

Yield strength of Graphene is N/A.

Modulus of Elasticity of Graphene

The Young’s modulus of elasticity of Graphene is 1000 GPa.

Hardness of Graphene

In materials science, hardness is the ability to withstand surface indentation (localized plastic deformation) and scratching. Brinell hardness test is one of indentation hardness tests, that has been developed for hardness testing. In Brinell tests, a hard, spherical indenter is forced under a specific load into the surface of the metal to be tested.

The Brinell hardness number (HB) is the load divided by the surface area of the indentation. The diameter of the impression is measured with a microscope with a superimposed scale. The Brinell hardness number is computed from the equation:

Brinell hardness of Graphene is approximately N/A.

See also: Hardness of Materials

Thermal Properties of Graphene

Graphene – Melting Point

Melting point of Graphene is 3697 °C.

Note that, these points are associated with the standard atmospheric pressure. 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 in which the solid and liquid can exist in equilibrium. For various chemical compounds and alloys, it is difficult to define the melting point, since they are usually a mixture of various chemical elements.

Graphene – Thermal Conductivity

Thermal conductivity of Graphene is 4000 W/(m·K).

The heat transfer characteristics of a solid material are measured by a property called the thermal conductivity, k (or λ), measured in W/m.K. It is a measure of a substance’s ability to transfer heat through a material by conduction. Note that Fourier’s law applies for 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. For vapors, it also depends upon pressure. In general:

Most materials are very 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.

Graphene – Specific Heat

Specific heat of Graphene is 509 J/g K.

Specific heat, or specific heat capacity, is a property related to internal energy that is very important in thermodynamics. The intensive properties c_v and c_p are defined for pure, simple compressible substances as partial derivatives of the internal energy u(T, v) and enthalpy h(T, p), respectively:

where the subscripts v and p denote the variables held fixed during differentiation. The properties c_v and c_p are referred to as specific heats (or heat capacities) because under certain special conditions they relate the temperature change of a system to the amount of energy added by heat transfer. Their SI units are J/kg K or J/mol K.

Properties and prices of other materials

material-table-in-8k-resolution