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- (Absolute) thermal resistance R in kelvins per watt (K/W) is a property of a particular component. For example, a characteristic of a heat sink.
- Specific thermal resistance or thermal resistivity Rλ in kelvin metres per watt (K⋅m/W), is a material constant.
- Thermal insulance has the units square metre kelvins per watt (m2⋅K/W) in SI units or square foot degree Fahrenheit hours per British thermal unit (ft2⋅°F⋅h/Btu) in imperial units. It is the thermal resistance of unit area of a material. In terms of insulation, it is measured by the R-value.
Absolute thermal resistance
Absolute thermal resistance is the temperature difference across a structure when a unit of heat energy flows through it in unit time. It is the reciprocal of thermal conductance. The SI unit of absolute thermal resistance is kelvins per watt (K/W) or the equivalent degrees Celsius per watt (°C/W) – the two are the same since the intervals are equal: ΔT = 1 K = 1 °C.
The thermal resistance of materials is of great interest to electronic engineers because most electrical components generate heat and need to be cooled. Electronic components malfunction or fail if they overheat, and some parts routinely need measures taken in the design stage to prevent this.
Electrical engineers are familiar with Ohm's law and so often use it as an analogy when doing calculations involving thermal resistance. Mechanical and structural engineers are more familiar with Hooke's law and so often use it as an analogy when doing calculations involving thermal resistance.
|type||structural analogy||hydraulic analogy||thermal||electrical analogy|
|quantity||... [N·s]||volume [m3]||heat [J]||charge [C]|
|potential||displacement [m]||pressure [N/m2]||temperature [K]||potential [V = J/C]|
|flux||load or force [N]||flow rate [m3/s]||heat transfer rate [W = J/s]||current [A = C/s]|
|flux density||stress [Pa = N/m2]||velocity [m/s]||heat flux [W/m2]||current density [C/(m2·s) = A/m2]|
|resistance||flexibility (rheology defined) [1/Pa]||fluid resistance [...]||thermal resistance [K/W]||electrical resistance [Ω]|
|conductance||... [Pa]||fluid conductance [...]||thermal conductance [W/K]||electrical conductance [S]|
|resistivity||flexibility [m/N]||fluid resistivity||thermal resistivity [(m·K)/W]||electrical resistivity [Ω·m]|
|conductivity||stiffness [N/m]||fluid conductivity||thermal conductivity [W/(m·K)]||electrical conductivity [S/m]|
|lumped element linear model||Hooke's law||Hagen–Poiseuille equation||Newton's law of cooling||Ohm's law|
|distributed linear model||...||...||Fourier's law||Ohm's law|
Explanation from an electronics point of view
Equivalent thermal circuits
The heat flow can be modelled by analogy to an electrical circuit where heat flow is represented by current, temperatures are represented by voltages, heat sources are represented by constant current sources, absolute thermal resistances are represented by resistors and thermal capacitances by capacitors.
The diagram shows an equivalent thermal circuit for a semiconductor device with a heat sink.
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Consider a component such as a silicon transistor that is bolted to the metal frame of a piece of equipment. The transistor's manufacturer will specify parameters in the datasheet called the absolute thermal resistance from junction to case (symbol: ), and the maximum allowable temperature of the semiconductor junction (symbol: ). The specification for the design should include a maximum temperature at which the circuit should function correctly. Finally, the designer should consider how the heat from the transistor will escape to the environment: this might be by convection into the air, with or without the aid of a heat sink, or by conduction through the printed circuit board. For simplicity, let us assume that the designer decides to bolt the transistor to a metal surface (or heat sink) that is guaranteed to be less than above the ambient temperature. Note: THS appears to be undefined.
Given all this information, the designer can construct a model of the heat flow from the semiconductor junction, where the heat is generated, to the outside world. In our example, the heat has to flow from the junction to the case of the transistor, then from the case to the metalwork. We do not need to consider where the heat goes after that, because we are told that the metalwork will conduct heat fast enough to keep the temperature less than above ambient: this is all we need to know.
Suppose the engineer wishes to know how much power he can put into the transistor before it overheats. The calculations are as follows.
- Total absolute thermal resistance from junction to ambient =
where is the absolute thermal resistance of the bond between the transistor's case and the metalwork. This figure depends on the nature of the bond - for example, a thermal bonding pad or thermal transfer grease might be used to reduce the absolute thermal resistance.
- Maximum temperature drop from junction to ambient = .
We use the general principle that the temperature drop across a given absolute thermal resistance with a given heat flow through it is:
Substituting our own symbols into this formula gives:
The designer now knows , the maximum power that the transistor can be allowed to dissipate, so he can design the circuit to limit the temperature of the transistor to a safe level.
Let us substitute some sample numbers:
- (typical for a silicon transistor)
- (a typical specification for commercial equipment)
- (for a typical TO-220 package)
- (a typical value for an elastomer heat-transfer pad for a TO-220 package)
- (a typical value for a heatsink for a TO-220 package)
The result is then:
This means that the transistor can dissipate about 18 watts before it overheats. A cautious designer would operate the transistor at a lower power level to increase its reliability.
This method can be generalised to include any number of layers of heat-conducting materials, simply by adding together the absolute thermal resistances of the layers and the temperature drops across the layers.
Derived from Fourier's Law for heat conduction
- is the absolute thermal resistance (K/W) across the thickness of the sample
- is the thickness (m) of the sample (measured on a path parallel to the heat flow)
- is the thermal conductivity (W/(K·m)) of the sample
- is the thermal resistivity (K·m/W) of the sample
- is the cross-sectional area (m2) perpendicular to the path of heat flow.
In terms of the temperature gradient across the sample and heat flux through the sample, the relationship is:
- is the absolute thermal resistance (K/W) across the thickness of the sample,
- is the thickness (m) of the sample (measured on a path parallel to the heat flow),
- is the heat flux through the sample (W·m−2),
- is the temperature gradient (K·m−1) across the sample,
- is the cross-sectional area (m2) perpendicular to the path of heat flow through the sample,
- is the temperature difference (K) across the sample,
- is the rate of heat flow (W) through the sample.
Problems with electrical resistance analogy
A 2008 review paper written by Philips researcher Clemens J. M. Lasance notes that: "Although there is an analogy between heat flow by conduction (Fourier’s law) and the flow of an electric current (Ohm’s law), the corresponding physical properties of thermal conductivity and electrical conductivity conspire to make the behavior of heat flow quite unlike the flow of electricity in normal situations. [...] Unfortunately, although the electrical and thermal differential equations are analogous, it is erroneous to conclude that there is any practical analogy between electrical and thermal resistance. This is because a material that is considered an insulator in electrical terms is about 20 orders of magnitude less conductive than a material that is considered a conductor, while, in thermal terms, the difference between an "insulator" and a "conductor" is only about three orders of magnitude. The entire range of thermal conductivity is then equivalent to the difference in electrical conductivity of high-doped and low-doped silicon."
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The junction-to-air thermal resistance can vary greatly depending on the ambient conditions. (A more sophisticated way of expressing the same fact is saying that junction-to-ambient thermal resistance is not Boundary-Condition Independent (BCI).) JEDEC has a standard (number JESD51-2) for measuring the junction-to-air thermal resistance of electronics packages under natural convection and another standard (number JESD51-6) for measurement under forced convection.
A JEDEC standard for measuring the junction-to-case thermal resistance (JESD51-14) is relatively newcomer, having been published in late 2010; it concerns only packages having a single heat flow and an exposed cooling surface.
Resistance in Composite Wall
Parallel thermal resistance
Similarly to electrical circuits, the total thermal resistance for steady state conditions can be calculated as follows.
The total thermal resistance
Simplifying the equation, we get
With terms for the thermal resistance for conduction, we get
Resistance in series and parallel
It is often suitable to assume one-dimensional conditions, although the heat flow is multidimensional. Now, two different circuits may be used for this case. For case (a) (shown in picture), we presume isothermal surfaces for those normal to the x- direction, whereas for case (b) we presume adiabatic surfaces parallel to the x- direction. We may obtain different results for the total resistance and the actual corresponding values of the heat transfer are bracketed by . When the multidimensional effects becomes more significant, these differences are increased with increasing .
Spherical and cylindrical systems may be treated as one-dimensional, due to the temperature gradients in the radial direction. The standard method can be used for analyzing radial systems under steady state conditions, starting with the appropriate form of the heat equation, or the alternative method, starting with the appropriate form of Fourier's law. For a hollow cylinder in steady state conditions with no heat generation, the appropriate form of heat equation is 
Where is treated as a variable. Considering the appropriate form of Fourier's law, the physical significance of treating as a variable becomes evident when the rate at which energy is conducted across a cylindrical surface, this is represented as
Where is the area that is normal to the direction of where the heat transfer occurs. Equation 1 implies that the quantity is not dependent of the radius , it follows from equation 5 that the heat transfer rate, is a constant in the radial direction.
In order to determine the temperature distribution in the cylinder, equation 4 can be solved applying the appropriate boundary conditions. With the assumption that is constant
Using the following boundary conditions, the constants and can be computed
The general solution gives us
Solving for and and substituting into the general solution, we obtain
The logarithmic distribution of the temperature is sketched in the inset of the thumbnail figure. Assuming that the temperature distribution, equation 7, is used with Fourier’s law in equation 5, the heat transfer rate can be expressed in the following form
Finally, for radial conduction in a cylindrical wall, the thermal resistance is of the form
- Tony Abbey. "Using FEA for Thermal Analysis". Desktop Engineering magazine. 2014 June. p. 32.
- "The Design of Heatsinks".
- Lasance, C. J. M. (2008). "Ten Years of Boundary-Condition- Independent Compact Thermal Modeling of Electronic Parts: A Review". Heat Transfer Engineering. 29 (2): 149–168. Bibcode:2008HTrEn..29..149L. doi:10.1080/01457630701673188.
- Ho-Ming Tong; Yi-Shao Lai; C.P. Wong (2013). Advanced Flip Chip Packaging. Springer Science & Business Media. pp. 460–461. ISBN 978-1-4419-5768-9.
- Younes Shabany (2011). Heat Transfer: Thermal Management of Electronics. CRC Press. pp. 111–113. ISBN 978-1-4398-1468-0.
- Clemens J.M. Lasance; András Poppe (2013). Thermal Management for LED Applications. Springer Science & Business Media. p. 247. ISBN 978-1-4614-5091-7.
- "Experiment vs. Simulation, Part 3: JESD51-14". 2013-02-22.
- Schweitzer, D.; Pape, H.; Chen, L.; Kutscherauer, R.; Walder, M. (2011). "Transient dual interface measurement — A new JEDEC standard for the measurement of the junction-to-case thermal resistance". 2011 27th Annual IEEE Semiconductor Thermal Measurement and Management Symposium. p. 222. doi:10.1109/STHERM.2011.5767204. ISBN 978-1-61284-740-5.
- Incropera, Dewitt, Bergman, Lavine, Frank P., David P., Theodore L., Adrienne S. (2013). Principles of Heat and Mass Transfer. John Wiley & Sons; 7th Edition, Interna edition. ISBN 978-0470646151.CS1 maint: multiple names: authors list (link)
- Michael Lenz, Günther Striedl, Ulrich Fröhler (January 2000) Thermal Resistance, Theory and Practice. Infineon Technologies AG, Munich, Germany.
- Directed Energy, Inc./IXYSRF (March 31, 2003) R Theta And Power Dissipation Technical Note. Ixys RF, Fort Collins, Colorado. Example thermal resistance and power dissipation calculation in semiconductors.
There is a large amount of literature on this topic. In general, works using the term "thermal resistance" are more engineering-oriented, whereas works using the term thermal conductivity are more [pure-]physics-oriented. The following books are representative, but may be easily substituted.
- Terry M. Tritt, ed. (2004). Thermal Conductivity: Theory, Properties, and Applications. Springer Science & Business Media. ISBN 978-0-306-48327-1.
- Younes Shabany (2011). Heat Transfer: Thermal Management of Electronics. CRC Press. ISBN 978-1-4398-1468-0.
- Xingcun Colin Tong (2011). Advanced Materials for Thermal Management of Electronic Packaging. Springer Science & Business Media. ISBN 978-1-4419-7759-5.
- Guoping Xu (2006), Thermal Management for Electronic Packaging, Sun Microsystems
- The importance of Soil Thermal Resistivity for power companies