Monday, February 11, 2013

Materials Engineering

II.THERMAL PROPERTIES

A. thermal conduction

 Thermal conduction, k, is the property of a strong reflecting its ability to conduct  affectionateness. It appears primarily in Fouriers Law for  rage conduction. Thermal conductivity is measured in watts per Kelvin per  pulsation (W·K?1·m?1). Multiplied by a temperature difference (in Kelvin, K) and an area (in square metres, m2), and divided by a thickness (in meters, m), the thermal conductivity predicts the rate of energy press release (in watts, W) through a piece of material.

The reciprocal of thermal conductivity is thermal resistivity. Usually measured in kelvin-metres per watt (K·m·W?1). When dealing with a known amount of material, its thermal conductance and the reciprocal property, thermal resistance, can be described. 

B. Thermal diffusity

Thermal diffusivity (symbol: [pic], but note that the symbols ?, D, and k are all usually used) is the thermal conductivity divided by the volumetrical genus Oestrus strength. It has the SI unit of m²/s.

[pic]
where:

? k : thermal conductivity (SI units: W/(m·K))
? ? : density (kg/m³)
? cp : specific heat strength (J/(kg·K))
Substances with high thermal diffusivity rapidly adjust their temperature to that of their surroundings, because they conduct heat quickly in comparison to their volumetric heat capacity or thermal bulk.

C.

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Thermal expansion

Thermal expansion is the tendency of military issue to change in volume in response to a change in temperature.[1] All materials have this tendency.

When a meat is heated, its particles begin moving and become active thus maintaining a greater average separation.

The change in the one-dimensional and volumetric dimension can be estimated to be:

?L = coefficient of linear expansion

L = initial length

?T= change in temperature

?L=change in length

?V= coefficient of volume expansion

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