Abstract
In this chapter, after a generic discussion of thermal testing techniques used to characterize packaged semiconductor devices; the latest practical test methods widespread in thermal testing of LED components and SSL luminaires are discussed. Thus, the focus is on the latest, power semiconductor and LED-specific test procedures, environments and thermal metrics—all derived from the classical JEDEC JESD51 family of testing standards. Detailed discussion is devoted to the transient extension of the so-called static test method and the differential measurement principle in its practical realization.
Different representations of the thermal impedance are presented starting from the classical Z th (t) functions ending with the so-called structure functions. These are discussed in depth because they became the de facto standard in laboratory testing of thermal properties of LED components, in reliability analysis and in quality assurance at leading LED manufacturers. The basic concepts are introduced through practical examples.
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Notes
- 1.
Some of these topics will be discussed later in this chapter and many more in Chap. 11, but their detailed treatment is beyond the scope of this book.
- 2.
The mentioned cities span over a large surface while distance is defined between two points. The question is: are there some points in these cities which are characteristic for the real target of the distance measurement and where are they located? We face similar questions in the thermal testing of semiconductor devices. To which point of the active semiconductor we assign the “junction temperature”? Resistance (strictly speaking) is defined between two nodes of a graph. Which are the distinct points between which we define the thermal resistance? See Chap. 6 for further details on these issues.
- 3.
- 4.
The junction-to-test point thermal characterization parameter is a thermal metric, which can help relate junction temperatures to test point temperatures. Discussion of such simple tests is not the main target of this chapter.
- 5.
- 6.
Voltage and current notations correspond to the notations used the JESD51-5x series of standards, see also Chap. 6.
- 7.
This extension was first defined in details in the JEDEC JESD 51-14 standard [13]. This proposes a transient method for the measurement of the junction-to-case thermal resistance of power semiconductor device packages with a single heat flow path and with an exposed cooling surface—such as power LED packages. JEDEC JESD 51-14 also prefers the cooling mode transient measurement for diodes since the error introduced by the slightly changing power after switching is negligible in this case (as we also pointed out by a numerical example). The most recent LED thermal testing standard JESD51-51 [6] also recommends the cooling mode measurement if the task is to measure the real Z th (t) thermal impedance of an LED package.
- 8.
See also Chap. 2 on the physical basics of LEDs.
- 9.
- 10.
- 11.
The concept of cumulative resistance and cumulative capacitance and the concept of the CΣ(RΣ) function were first introduced by Protonotarios and Wing in their fundamental papers about the theory of nonuniform (electrical) RC lines. In the first part, Protonotarios, E. N. [22] they used this function for simplifying the telegraphists’ equations when used in the synthesis of nonuniform RC lines.
- 12.
- 13.
Achieving a time resolution higher than 20 points per decade may require unaffordable simulation resources while measuring a thermal transient with about 200 or 400 points per decade resolution is not a problem with the transient extension of the JESD51-1 “static” test method.
- 14.
This problem can be overcome by using special math libraries in the implementation, which provide any number of digits both for the exponent and for the mantissa.
- 15.
In many cases, the adjective “cumulative” is neglected and the CSF is simply called the structure function.
- 16.
The analysis technique based on changing C th /R th ratio in the structure function was first suggested by Rencz et al. [29] for the study of die attach voiding and for TIM quality assessment.
- 17.
In this particular case, about 1.5 % loss can be attributed directly to the increased thermal resistance.
- 18.
Measurement and simulation results by courtesy of Vass-Várnai and Bornoff.
- 19.
These ballasts usually hamper thermal testing and thus need to be bypassed for the sake of this test.
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Farkas, G., Poppe, A. (2014). Thermal Testing of LEDs. In: Lasance, C., Poppe, A. (eds) Thermal Management for LED Applications. Solid State Lighting Technology and Application Series, vol 2. Springer, New York, NY. https://doi.org/10.1007/978-1-4614-5091-7_4
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