- Thermal conductivity
In

physics ,**thermal conductivity**, $k$, is the property of a material that indicates its ability to conductheat . It appears primarily in Fourier's Law forheat conduction .First, we define

heat conduction by the formula::: $H=frac\{Delta\; Q\}\{Delta\; t\}=k\; imes\; A\; imesfrac\{Delta\; T\}\{x\}$where $frac\{Delta\; Q\}\{Delta\; t\}$ is the rate of heat flow, "k" is the thermal conductivity, "A" is the total cross sectional area of conducting surface, Δ"T" is temperature difference and "x" is the thickness of conducting surface separating the 2 temperatures.Thus, rearranging the equation gives thermal conductivity,

:: $k=frac\{Delta\; Q\}\{Delta\; t\}\; imesfrac\{1\}\{A\}\; imesfrac\{x\}\{Delta\; T\}$

(Note: $frac\{Delta\; T\}\{x\}$ is the temperature gradient)

In other words, it is defined as the quantity of heat, Δ"Q", transmitted during time Δ"t" through a thickness "x", in a direction normal to a surface of area "A", due to a temperature difference Δ"T", under steady state conditions and when the heat transfer is dependent only on the temperature gradient.

Alternatively, it can be thought of as a

flux of heat (energy per unit area per unit time) divided by a temperature gradient (temperature difference per unit length):: $k=frac\{Delta\; Q\}\{A\; imes\{\}\; Delta\; t\}\; imesfrac\{x\}\{Delta\; T\}$

Typical units are

SI : W/(m·K) andEnglish units : Btu·ft/(h·ft²·°F). To convert between the two, use the relation 1 Btu·ft/(h·ft²·°F) = 1.730735 W/(m·K). [Perry's Chemical Engineers' Handbook, 7th Edition, Table 1-4]**Examples**In

metal s, thermal conductivity approximately trackselectrical conductivity according to theWiedemann-Franz law , as freely movingvalence electron s transfer not only electric current but also heat energy. However, the general correlation between electrical and thermal conductance does not hold for other materials, due to the increased importance ofphonon carriers for heat in non-metals. As shown in the table below, highly electrically conductivesilver is less thermally conductive thandiamond , which is anelectrical insulator .Thermal conductivity depends on many properties of a material, notably its structure and temperature. For instance, pure

crystalline substances exhibit very different thermal conductivities along different crystal axes, due to differences in phonon coupling along a given crystal axis.Sapphire is a notable example of variable thermal conductivity based on orientation and temperature, for which the [*http://www.hbcpnetbase.com/ CRC Handbook*] reports a thermal conductivity of 2.6 W/(m·K) perpendicular to the "c"-axis at 373 K, but 6000 W/(m·K) at 36 degrees from the "c"-axis and 35 K.Air and other gases are generally good insulators, in the absence of

convection . Therefore, many insulating materials function simply by having a large number of gas-filled pockets which prevent large-scale convection. Examples of these include expanded and extrudedpolystyrene (popularly referred to as "styrofoam") and silicaaerogel . Natural, biological insulators such as fur andfeathers achieve similar effects by dramatically inhibiting convection of air or water near an animal's skin.Thermal conductivity is important in

building insulation and related fields. However, materials used in such trades are rarely subjected to chemical purity standards. Several construction materials' "k" values are listed below. These should be considered approximate due to the uncertainties related to material definitions.The following table is meant as a small sample of data to illustrate the thermal conductivity of various types of substances. For more complete listings of measured "k"-values, see the references.

**List of thermal conductivity values**This is a list of approximate values of thermal conductivity, "k", for some common materials. Please consult the

list of thermal conductivities for more accurate values, references and detailed information.**Measurement**Generally speaking, there are a number of possibilities to measure thermal conductivity, each of them suitable for a limited range of materials, depending on the thermal properties and the medium temperature. There can be made a distinction between steady-state and transient techniques.

In general the steady-state techniques perform a measurement when the temperature of the material that is measured does not change with time. This makes the signal analysis straight forward (steady state implies constant signals). The disadvantage generally is that it takes a well-engineered experimental setup. The Divided Bar (various types) is the most common device used for consolidated rock samples.

The transient techniques perform a measurement during the process of heating up. The advantage is that measurements can be made relatively quickly. Transient methods are usually carried out by needle probes (inserted into samples or plunged into the ocean floor).

For good conductors of heat,

Searle's bar method can be used. [*http://media.paisley.ac.uk/~davison/labpage/searle/searle.html*] For poor conductors of heat,Lees' disc method can be used. [*http://academia.hixie.ch/bath/Thermal/home.html*] An alternative traditional method using real thermometers is described at [*http://www.uow.edu.au/eng/phys/200labs/phys235/badcon.pdf*] . A brief review of new methods measuring thermal conductivity,thermal diffusivity and specific heat within a single measurement is available at [*http://thermophys.savba.sk/Methods.htm*] .A thermal conductance tester, one of the instruments ofgemology , determines if gems are genuinediamond s using diamond's uniquely high thermal conductivity.**tandard Measurement Techniques***IEEE Standard 442-1981, "IEEE guide for soil thermal resistivity measurements" see als

soil thermal properties [*http://ieeexplore.ieee.org/servlet/opac?punumber=2543*]*IEEE Standard 98-2002, "Standard for the Preparation of Test Procedures for the Thermal Evaluation of Solid Electrical Insulating Materials", ISBN 0-7381-3277-2 [

*http://ieeexplore.ieee.org/servlet/opac?punumber=7893*]*ASTM Standard D5470-06, "Standard Test Method for Thermal Transmission Properties of Thermally Conductive Electrical Insulation Materials" [

*http://www.astm.org/cgi-bin/SoftCart.exe/DATABASE.CART/REDLINE_PAGES/D5470.htm?E+mystore*]*ASTM Standard E1225-04, "Standard Test Method for Thermal Conductivity of Solids by Means of the Guarded-Comparative-Longitudinal Heat Flow Technique" [

*http://www.astm.org/cgi-bin/SoftCart.exe/DATABASE.CART/REDLINE_PAGES/E1225.htm?L+mystore+wnox2486+1189558298*]*ASTM Standard D5930-01, "Standard Test Method for Thermal Conductivity of Plastics by Means of a Transient Line-Source Technique" [

*http://www.astm.org/cgi-bin/SoftCart.exe/STORE/filtrexx40.cgi?U+mystore+wnox2486+-L+THERMAL:CONDUCTIVITY+/usr6/htdocs/astm.org/DATABASE.CART/REDLINE_PAGES/D5930.htm*]*ASTM Standard D2717-95, "Standard Test Method for Thermal Conductivity of Liquids" [

*http://www.astm.org/cgi-bin/SoftCart.exe/DATABASE.CART/REDLINE_PAGES/D2717.htm?L+mystore+wnox2486+1189564966*]**Difference between US and European notation**What is called the k-value of construction materials (e.g. window glass) in the US, is called λ-value in Europe.

What is called U-value (= the inverse of R-value) in the US, used to be called k-value in Europe, but is now also called U-value in Europe.

**K-value**(with capital k) refers in Europe to the total isolation value of a building. K-value is obtained by multiplying theform factor of the building (= the total inward surface of the outward walls of the building divided by the total volume of the building) with the average U-value of the outward walls of the building. K-value is therefore expressed as (m^{2}.m^{-3}).(W.K^{-1}.m^{-2}) = W.K^{-1}.m^{-3}. A house with a volume of 400 m³ and a K-value of 0.45 (the new European norm. It is commonly referred to as K45) will therefore theoretically require 180 W to maintain its interior temperature 1 degree K above exterior temperature. So, to maintain the house at 20°C when it is freezing outside (0°C), 3600 W of continuous heating is required.**Related terms**The reciprocal of thermal conductivity is "thermal resistivity", measured in

kelvin -metre s perwatt (K·m·W^{−1}).When dealing with a known amount of material, its "thermal conductance" and the reciprocal property, "thermal resistance", can be described. Unfortunately there are differing definitions for these terms.

**Thermal Conductance**For general scientific use, "thermal conductance" is the quantity of heat that passes in unit time through a plate of "particular area and thickness" when its opposite faces differ in temperature by one degree. For a plate of thermal conductivity "k", area "A" and thickness "L" this is "kA/L", measured in W·K

^{−1}(equivalent to: W/°C). Thermal conductivity and conductance are analogous toelectrical conductivity (A·m^{−1}·V^{−1}) andelectrical conductance (A·V^{−1}).There is also a measure known as

heat transfer coefficient : the quantity of heat that passes in unit time through "unit area" of a plate of particular thickness when its opposite faces differ in temperature by one degree. The reciprocal is "thermal insulance". In summary:

*"thermal conductance" = "kA"/"L", measured in W·K^{−1}

** "thermal resistance" = "L"/"kA", measured in K·W^{−1}(equivalent to: °C/W)

*"heat transfer coefficient" = "k"/"L", measured in W·K^{−1}·m^{−2}

**"thermal insulance" = "L"/"k", measured in K·m²·W^{−1}.The heat transfer coefficient is also known as "thermal admittance"

**Thermal Resistance**When thermal resistances occur in

series , they are additive. So when heat flows through two components each with a resistance of 1 °C/W, the total resistance is 2 °C/W.A common engineering design problem involves the selection of an appropriate sized

heat sink for a given heat source. Working in units of thermal resistance greatly simplifies the design calculation. The following formula can be used to estimate the performance::$R\_\{hs\}\; =\; frac\; \{Delta\; T\}\{P\_\{th\; -\; R\_s$ where:

* R_{hs}is the maximum thermal resistance of the heat sink to ambient, in °C/W

* $Delta\; T$ is the temperature difference (temperature drop), in °C

* P_{th}is the thermal power (heat flow), in Watts

* R_{s}is the thermal resistance of the heat source, in °C/WFor example, if a component produces 100 W of heat, and has a thermal resistance of 0.5 °C/W, what is the maximum thermal resistance of the heat sink? Suppose the maximum temperature is 125 °C, and the ambient temperature is 25 °C; then the $Delta\; T$ is 100 °C. The heat sink's thermal resistance to ambient must then be 0.5 °C/W or less.

**Alternate definition (buildings)**When dealing with buildings, "thermal resistance" or "R-value" means what is described above as thermal insulance, and "thermal conductance" means the reciprocal. For materials in series, these thermal resistances (unlike conductances) can simply be added to give a thermal resistance for the whole.

A third term, "thermal transmittance", incorporates the thermal conductance of a structure along with heat transfer due to

convection and radiation. It is measured in the same units as thermal conductance and is sometimes known as the "composite thermal conductance". The term "U-value" is another synonym.In summary, for a plate of thermal conductivity "k" (the "k value" [

*[*] ), area "A" and thickness "L":*http://www.plastics.org.nz/page.asp?id=468 Definition of "k value" from Plastics New Zealand*]*"thermal conductance" = "k"/"L", measured in W·K

^{−1}·m^{−2};

*"thermal resistance" ("R value") = "L"/"k", measured in K·m²·W^{−1};

*"thermal transmittance" ("U value") = 1/(Σ("L"/"k")) +convection + radiation, measured in W·K^{−1}·m^{−2}.**Textile industry**In textiles, a tog value may be quoted as a measure of thermal resistance in place of a measure in SI units.

**Origins**The thermal conductivity of a system is determined by how atoms comprising the system interact. There are no simple, correct expressions for thermal conductivity. There are two different approaches for calculating the thermal conductivity of a system.

The first approach employs the

Green-Kubo relations . Although this employs analytic expressions which in principle can be solved, in order to calculate the thermal conductivity of a dense fluid or solid using this relation requires the use of molecular dynamics computer [*http://rsc.anu.edu.au/~evans/evansmorrissbook.htm simulation*] .The second approach is based upon the relaxation time approach. Due to the anharmonicity within the crystal potential, the

phonon s in the system are known to scatter. There are three main mechanisms for scattering:

*Boundary scattering, a phonon hitting the boundary of a system;

*Mass defect scattering, a phonon hitting an impurity within the system and scattering;

*Phonon-phonon scattering, a phonon breaking into two lower energy phonons or a phonon colliding with another phonon and merging into one higher energy phonon.Further information can be found in the publication "The Physics of Phonons" by G P Srivastava.

**ee also**

*Heat conduction

*Heat transfer

* Heat transfer mechanisms

*Insulated pipes

* R-value

*Specific Heat

*Thermal bridge

*Thermal contact conductance

*Thermal diffusivity

*Thermal resistance in electronics

*Thermistor

*Thermocouple

*Electrical conductivity **External links*** [

*http://environmentalchemistry.com/yogi/periodic/thermal.html Table with the Thermal Conductivity of the Elements*]

*http://physics.nist.gov/Pubs/SP811/appenB9.html

*http://www.npl.co.uk/thermal/faq_index.html#heat%20transfer%20property thermophysics FAQ5

*http://www.ornl.gov/roofs+walls/research/detailed_papers/rastra/dynamic.htm

*http://www.tak2000.com/data2.htm

*http://thermophys.savba.sk

* [*http://glassproperties.com/thermal-conductivity/ Calculation of the Thermal Conductivity of Glass*] Calculation of the Thermal Conductivity of Glass at Room Temperature from the Chemical Composition

*http://www.mathisinstruments.com/index.asp?pathinfo=/html/content/technology/tech_glossary.asp&dbbypass=

* [*http://www.boulder.nist.gov/div838/theory/refprop/NAO.PDF Viscosity and Thermal Conductivity Equations for Nitrogen, Oxygen, Argon, and Air*]**References***

* Halliday, David; Resnick, Robert; & Walker, Jearl(1997). "Fundamentals of Physics" (5th ed.). John Wiley and Sons, INC., NY ISBN 0-471-10558-9.

* TM 5-852-6 AFR 88-19, Volume 6 (Army Corp of Engineers publication)

* Srivastava G. P (1990), "The Physics of Phonons." Adam Hilger, IOP Publishing Ltd, Bristol.

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