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Journal articles on the topic 'Thermal conductivity measurements'

Author: Grafiati

Published: 4 June 2021

Last updated: 10 February 2022

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1

Pryazhnikov, M. I., A. V. Minakov, V. Ya Rudyak, and D. V. Guzei. "Thermal conductivity measurements of nanofluids." International Journal of Heat and Mass Transfer 104 (January 2017): 1275–82. http://dx.doi.org/10.1016/j.ijheatmasstransfer.2016.09.080.

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2

Cheruparambil, K. R., B. Farouk, J. E. Yehoda, and N. A. Macken. "Thermal Conductivity Measurement of CVD Diamond Films Using a Modified Thermal Comparator Method." Journal of Heat Transfer 122, no. 4 (May 9, 2000): 808–16. http://dx.doi.org/10.1115/1.1318206.

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Results from an experimental study on the rapid measurement of thermal conductivity of chemical vapor deposited (CVD) diamond films are presented. The classical thermal comparator method has been used successfully in the past for the measurement of thermal conductivity of bulk materials having high values of thermal resistance. Using samples of known thermal conductivity, a calibration curve is prepared. With this calibration curve, the comparator can be used to determine thermal conductivity of unknown samples. We have significantly modified and extended this technique for the measurement of materials with very low thermal resistance, i.e., CVD diamond films with high thermal conductivity. In addition to the heated probe, the modified comparator employs a thermoelectric cooling element of increase conductive heat transfer through the film. The thermal conductivity measurements are sensitive to many other factors such as the thermal contact resistances, anisotropic material properties, surrounding air currents and temperature, and ambient humidity. A comprehensive numerical model was also developed to simulate the heat transfer process for the modified comparator. The simulations were used to develop a “numerical” calibration curve that agreed well with the calibration curve obtained from our measurements. The modified method has been found to successfully measure the thermal conductivity of CVD diamond films. [S0022-1481(00)00804-5]

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3

Blows, J. L., P. Dekker, P. Wang, J. M. Dawes, and T. Omatsu. "Thermal lensing measurements and thermal conductivity of Yb:YAB." Applied Physics B: Lasers and Optics 76, no. 3 (March 1, 2003): 289–92. http://dx.doi.org/10.1007/s00340-002-1092-4.

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4

Twitchen, D. J., C. S. J. Pickles, S. E. Coe, R. S. Sussmann, and C. E. Hall. "Thermal conductivity measurements on CVD diamond." Diamond and Related Materials 10, no. 3-7 (March 2001): 731–35. http://dx.doi.org/10.1016/s0925-9635(00)00515-x.

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5

Goodrich, L. E. "Field measurements of soil thermal conductivity." Canadian Geotechnical Journal 23, no. 1 (February 1, 1986): 51–59. http://dx.doi.org/10.1139/t86-006.

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Data representing the seasonal variation of thermal conductivity of the ground at depths within the seasonally active freezing/thawing zone are presented for a number of different soil conditions at four sites across Canada. An inexpensive probe apparatus suitable for routine field measurements is described.In all the cases examined, significant seasonal variations were confined to the first few decimetres. In addition to distinct seasonal differences associated with phase change, quite large changes occurred during the period when the soil was thawed in those cases where seasonal drying was possible. Below the seasonally active zone, thawed soil conductivities did not differ greatly among the three nonpermafrost sites in spite of soil composition ranging from marine clay to sandy silt. The data suggest that, even within a given soil layer, quite significant differences in thermal conductivity may be encountered in engineering structures such as embankments, presumably because of differences in drainage conditions. Key words: thermal conductivity, field measurements, phase relationships, drying, permafrost, clay, silt, peat.

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6

Sturm, Matthew, and Jerome B. Johnson. "Thermal conductivity measurements of depth hoar." Journal of Geophysical Research: Solid Earth 97, B2 (February 10, 1992): 2129–39. http://dx.doi.org/10.1029/91jb02685.

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7

Balaya, P., H. S. Jayanna, Hemant Joshi, G. Sumana, V. G. Narasimha Murthy, V. Prasad, and S. V. Subramanyam. "Thermal conductivity measurements at low temperatures." Bulletin of Materials Science 18, no. 8 (December 1995): 1007–11. http://dx.doi.org/10.1007/bf02745187.

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8

Buliński, Z., S. Pawlak, T. Krysiński, W. Adamczyk, and R. Białecki. "Application of the ASTM D5470 standard test method for thermal conductivity measurements of high thermal conductive materials." Journal of Achievements in Materials and Manufacturing Engineering 2, no. 95 (August 1, 2019): 57–63. http://dx.doi.org/10.5604/01.3001.0013.7915.

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Purpose: The purpose of the present study was to demonstrate the procedure for determining the thermal conductivity of a solid material with relatively high thermal conductivity, using an original self-designed apparatus. Design/methodology/approach: The thermal conductivity measurements have been performed according to the ASTM D5470 standard. The thermal conductivity was calculated from the recorded temperature values in steady-state heat transfer conditions and determined heat flux. Findings: It has been found from the obtained experimental results that the applied standard test method, which was initially introduced for thermal conductivity measurements of thermal interface materials (TIMs), is also suitable for materials with high thermal conductivity, giving reliable results. Research limitations/implications: The ASTM D5470 standard test method for measurement of thermal conductivity usually gives poor results for high conductive materials having thermal conductivity above 100 W/mK, due to problems with measuring heat flux and temperature drop across the investigated sample with reasonably high accuracy. Practical implications: The results obtained for the tested material show that the presented standard test method can also be used for materials with high thermal conductivity, which is of importance either for the industrial or laboratory applications. Originality/value: The thermal conductivity measurements have been carried out using an original self-designed apparatus, which was developed for testing broad range of engineering materials with high accuracy.

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9

Suhad Dawood Salman, Dr. Khalid Mershed, and Mr. Aoday Hatem. "New formula for predication thermal conductivity for homologous alkanes series function of carbon number." journal of the college of basic education 14, no. 62 (October 10, 2019): 125–39. http://dx.doi.org/10.35950/cbej.v14i62.4738.

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The main aim of this paper is to establish a correlation for prediction the thermal conductivity of n-alkanes within a give temperature range for homologous n-alkanes series from CH4 to C30H62. The predicted thermal conductivity values depend on the temperature and carbon number for each alkanes component. This paper describes a method of predicting the thermal conductivity of any alkanes between the temperature range, based on a measurement of the thermal conductivity. Where prediction are based on lower temperature measurements, where the accuracy is generally better then 3.1% for 178 data points. Useful predictions can also be made from any temperature measurements for most alkanes, but with reduced accuracy. This method permits alkanes to be used in situations where the thermal conductivity is important without having to make (or find) direct measurements over the entire temperature range of interest. Recommended thermal conductivity values are presented for 30 components.

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10

Hotra, Oleksandra, Svitlana Kovtun, Oleg Dekusha, and Żaklin Grądz. "Prospects for the Application of Wavelet Analysis to the Results of Thermal Conductivity Express Control of Thermal Insulation Materials." Energies 14, no. 17 (August 24, 2021): 5223. http://dx.doi.org/10.3390/en14175223.

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This article discusses an express control method that allows in situ measurements of the thermal conductivity of insulation materials. Three samples of the most common thermal insulation materials, such as polyurethane, extruded polystyrene, and expanded polystyrene, were studied. Additionally, optical and organic glasses were investigated as materials with a stable value of thermal conductivity. For the measurement of thermal conductivity, the express control device, which implements the differential method of local heat influence, was used. The case studies were focused on the reduction of fluctuations of the measured signals caused by different influencing factors using wavelet transform. The application of wavelet transform for data processing decreased the thermal conductivity measurement’s relative error for organic glass SOL and optical glasses TF-1 and LK-5. The application of wavelet transform thermal conductivity measurement data for polyurethane, extruded polystyrene, and expanded polystyrene allowed to reduce twice the duration of express control while maintaining the same level of measurement error. The results of the investigation could be used to increase the accuracy in express control of the thermal conductivity of insulation materials by improving the data processing. This approach could be implemented in software and does not require a change in the design of the measuring equipment or the use of additional tools.

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11

Wang, Xinwei, Baratunde A. Cola, Thomas L. Bougher, Stephen L. Hodson, Timothy S. Fisher, and Xianfan Xu. "PHOTOACOUSTIC TECHNIQUE FOR THERMAL CONDUCTIVITY AND THERMAL INTERFACE MEASUREMENTS." Annual Review of Heat Transfer 16, no. 1 (2013): 135–57. http://dx.doi.org/10.1615/annualrevheattransfer.v16.50.

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12

Zhao, Yansong, Yingpeng Zhen, Bjørn Petter Jelle, and Tobias Boström. "Measurements of ionic liquids thermal conductivity and thermal diffusivity." Journal of Thermal Analysis and Calorimetry 128, no. 1 (November 2, 2016): 279–88. http://dx.doi.org/10.1007/s10973-016-5881-0.

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13

Kim, Gwantaek, Moojoong Kim, and Hyunjung Kim. "Feasibility of Novel Rear-Side Mirage Deflection Method for Thermal Conductivity Measurements." Sensors 21, no. 17 (September 6, 2021): 5971. http://dx.doi.org/10.3390/s21175971.

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Among the noncontact measurement technologies used to acquire thermal property information, those that use the photothermal effect are attracting attention. However, it is difficult to perform measurements for new materials with different optical and thermal properties, owing to limitations of existing thermal conductivity measurement methods using the photothermal effect. To address this problem, this study aimed to develop a rear-side mirage deflection method capable of measuring thermal conductivity regardless of the material characteristics based on the photothermal effect. A thin copper film (of 20 µm thickness) was formed on the surfaces of the target materials so that measurements could not be affected by the characteristics of the target materials. In addition, phase delay signals were acquired from the rear sides of the target materials to exclude the influence of the pump beam, which is a problem in existing thermal conductivity measurement methods that use the photothermal effect. To verify the feasibility of the proposed measurement technique, thermal conductivity was measured for copper, aluminum, and stainless steel samples with a 250 µm thickness. The results were compared with literature values and showed good agreement with relative errors equal to or less than 0.2%.

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14

Graebner, J. E., and K. Azar. "Thermal Conductivity Measurements in Printed Wiring Boards." Journal of Heat Transfer 119, no. 3 (August 1, 1997): 401–5. http://dx.doi.org/10.1115/1.2824111.

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The effective thermal conductivity κ of multilayer printed wiring boards (PWBs) has been measured for heat flowing in a direction either parallel (κ∥) or perpendicular (κ⊥) to the plane of the board. The conductivity of the glass/epoxy insulating material from which the boards are manufactured is anisotropic (κ∥ge ≈ 3 × κ⊥ge) and nearly three orders of magnitude smaller than the conductivity of copper. This large difference between glass/epoxy and copper produces extremely high anisotropy in PWBs that contain continuous layers of copper. For such boards, values of the board-averaged conductivity in the two directions can differ by a factor of ~100 or more. The value of κ∥ is found to depend on the ratio of the total thickness of continuous layers of copper to the total thickness of glass/epoxy, while it depends hardly at all on the amount of copper circuitry visible on the surface.

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15

Galgaro, Antonio, Matteo Cultrera, Giorgia Dalla Santa, and Fabio Peron. "Laboratory thermal conductivity measurements on gravel sample." Acque Sotterranee - Italian Journal of Groundwater 7, no. 3 (September 25, 2018): 67–70. http://dx.doi.org/10.7343/as-2018-344.

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Modern Ground Source Heat Pumps (GSHPs) systems must be designed by taking into account the ground thermal properties, in order to properly plan the capability of the heat pumps to transfer calories through the Ground Source Heat Exchangers (GSHE) to the subsoil (and vice versa). [...]

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16

Kushino, Akihiro, Yiner Chen, and Masataka Ohkubo. "Thermal Conductivity Measurements for Superconducting Mass Spectrometry." Netsu Bussei 21, no. 2 (2007): 81–85. http://dx.doi.org/10.2963/jjtp.21.81.

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17

Matsuzaki, H., K. Hida, N. Kase, T. Nakano, and N. Takeda. "Thermal Conductivity Measurements of Caged Structural Superconductors." Physics Procedia 81 (2016): 61–64. http://dx.doi.org/10.1016/j.phpro.2016.04.025.

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18

Sawkey, D., V. Goudon, O. Buu, L. Puech, and P. E. Wolf. "Thermal conductivity measurements of polarized liquid He." Physica B: Condensed Matter 329-333 (May 2003): 118–19. http://dx.doi.org/10.1016/s0921-4526(02)01914-2.

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19

Nikończuk, Piotr. "Preliminary Measurements of Overspray Sediment’s Thermal Conductivity." OCHRONA PRZED KOROZJĄ 1, no. 2 (February 5, 2018): 14–16. http://dx.doi.org/10.15199/40.2018.2.3.

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20

Kuznetsov, Ivan, Ivan Mukhin, Dmitry Silin, and Oleg Palashov. "Thermal conductivity measurements using phase-shifting interferometry." Optical Materials Express 4, no. 10 (September 29, 2014): 2204. http://dx.doi.org/10.1364/ome.4.002204.

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21

Gaal, P. S., M. A. Thermitus, and Daniela E. Stroe. "Thermal conductivity measurements using the flash method." Journal of Thermal Analysis and Calorimetry 78, no. 1 (2004): 185–89. http://dx.doi.org/10.1023/b:jtan.0000042166.64587.33.

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22

Perkins, R. A., A. Laesecke, and C. A. Nieto de Castro. "Polarized transient hot wire thermal conductivity measurements." Fluid Phase Equilibria 80 (November 1992): 275–86. http://dx.doi.org/10.1016/0378-3812(92)87074-w.

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23

Chu, Dachen, Maxat Touzelbaev, Kenneth E. Goodson, Sergey Babin, and R. Fabian Pease. "Thermal conductivity measurements of thin-film resist." Journal of Vacuum Science & Technology B: Microelectronics and Nanometer Structures 19, no. 6 (2001): 2874. http://dx.doi.org/10.1116/1.1421557.

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24

Fiege, Gero Bernhard Martin, Andreas Altes, Ralf Heiderhoff, and Ludwig Josef Balk. "Quantitative thermal conductivity measurements with nanometre resolution." Journal of Physics D: Applied Physics 32, no. 5 (January 1, 1999): L13—L17. http://dx.doi.org/10.1088/0022-3727/32/5/003.

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25

Hickox, C. E., D. F. McVey, J. B. Miller, L. O. Olson, and A. J. Silva. "Thermal conductivity measurements of pacific illite sediment." International Journal of Thermophysics 7, no. 4 (July 1986): 755–64. http://dx.doi.org/10.1007/bf00503833.

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26

Tuliszka, Marek, and Feliks Jaroszyk. "Thermal conductivity measurements of tRNA melting process." Thermochimica Acta 219 (May 1993): 355–60. http://dx.doi.org/10.1016/0040-6031(93)80512-9.

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27

Goodson, K. E., and M. I. Flik. "Solid Layer Thermal-Conductivity Measurement Techniques." Applied Mechanics Reviews 47, no. 3 (March 1, 1994): 101–12. http://dx.doi.org/10.1115/1.3111073.

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The thermal conductivities of solid layers of thicknesses from 0.01 to 100 μm affect the performance and reliability of electronic circuits, laser systems, and microfabricated sensors. This work reviews techniques that measure the effective thermal conductivity along and normal to these layers. Recent measurements using microfabricated experimental structures show the importance of measuring the conductivities of layers that closely resemble those in the application. Several promising non-contact techniques use laser light for heating and infrared detectors for temperature measurements. For transparent layers these methods require optical coatings whose impact on the measurements has not been determined. There is a need for uncertainty analysis in many cases, particularly for those techniques which apply to very thin layers or to layers with very high conductivities.

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28

Henon, J., A. Alzina, J. Absi, D. S. Smith, and S. Rossignol. "Analytical estimation of skeleton thermal conductivity of a geopolymer foam from thermal conductivity measurements." European Physical Journal Special Topics 224, no. 9 (July 2015): 1715–23. http://dx.doi.org/10.1140/epjst/e2015-02493-8.

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29

Zhang, Xing, and Motoo Fujii. "Measurements of the thermal conductivity and thermal diffusivity of polymers." Polymer Engineering & Science 43, no. 11 (November 2003): 1755–64. http://dx.doi.org/10.1002/pen.10148.

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30

Hütter, E. S., and N. I. Kömle. "Performance of thermal conductivity probes for planetary applications." Geoscientific Instrumentation, Methods and Data Systems Discussions 2, no. 1 (January 5, 2012): 23–86. http://dx.doi.org/10.5194/gid-2-23-2012.

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Abstract. This work aims to contribute to the development of in situ instruments feasible for space application. Commercial as well as custom made thermal sensors, based on the transient hot wire technique and suitable for direct measurement of the effective thermal conductivity of granular media, were tested for application under airless conditions. The investigated media range from compact specimen of well known thermal conductivity used for calibration of the sensors to various granular planetary analogue materials of different shape and grain size. Measurements were performed under gas pressures ranging from 103 hPa down to about 10−5 hPa. It was found that for the inspected granular materials the given pressure decrease results in a decrease of the thermal conductivity by about two orders of magnitude. In order to check the ability of custom-made sensors to measure the thermal conductivity of planetary surface layers, detailed numerical simulations predicting the response of the different sensors have also been performed. Both, measurements and simulations, revealed that for investigations under high vacuum conditions (as they prevail e.g. on the lunar surface) the derived thermal conductivity values can significantly depend on the sensor geometry, the axial heat flow and the thermal contact between probe and surrounding material. Therefore in these cases a careful calibration of each particular sensor is necessary in order to obtain reliable thermal conductivity measurements. The custom-made sensors presented in this work can serve as prototypes for payload to be flown on future planetary lander missions, in particular for airless bodies like the Moon, asteroids and comets, but also for Mars.

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31

Sattler, Pamela, and D. G. Fredlund. "Use of thermal conductivity sensors to measure matric suction in the laboratory." Canadian Geotechnical Journal 26, no. 3 (August 1, 1989): 491–98. http://dx.doi.org/10.1139/t89-063.

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The measurement of soil suction is pivotal to the application of soil mechanics principles in geotechnical engineering practice related to unsaturated soils. Volume change, shear strength, and seepage analyses all require an understanding of the matric suction in the soil. This note summarizes the use of thermal conductivity sensors to measure matric suction in the laboratory. The thermal conductivity sensor is described along with its mode of operation. A brief description is given of the procedure for calibrating thermal conductivity sensors using a pressure plate apparatus. The measurement of matric suction can be performed in the laboratory on Shelby tube samples. The laboratory measurements of matric suction can be adjusted for the effect of overburden pressure in the field. The required equilibration time for suction measurements is discussed along with details of the test procedure. The applications of the measured suction values to design are briefly discussed.Key words: matric suction, negative pore-water pressure, thermal conductivity sensor, laboratory, undisturbed samples.

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32

Naugle, D. G., B. I. Belevtsev, and B. D. Hennings. "Magnetic Superconductors: Thermal Conductivity Studies." International Journal of Modern Physics B 17, no. 18n20 (August 10, 2003): 3454–57. http://dx.doi.org/10.1142/s0217979203021198.

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The coexistence of magnetic and superconducting order in rare-earth-nickel-borocarbides ( RNi 2 B 2 C with R = Tm, Er, Ho, Dy ) and in Ru-2122 rutheno-cuprates ( R = Eu and Gd) has been recently reported. Thermal conductivity measurements for magnetic superconductors from these families are discussed.

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33

Bai, Xuemei, and David E. Pegg. "Thermal Property Measurements on Biological Materials at Subzero Temperatures." Journal of Biomechanical Engineering 113, no. 4 (November 1, 1991): 423–29. http://dx.doi.org/10.1115/1.2895422.

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The self-heated thermistor technique was used to measure the thermal conductivity and thermal diffusivity of biomaterials at low temperatures. Thermal standards were selected to calibrate the system at temperatures from −10°C to −70°C. The thermal probes were constructed with a convection barrier which eliminates convection inside liquid samples of low viscosity, without affecting the conductivity and diffusivity results. Using this technique, the thermal conductivity and diffusivity of two organ perfusates (HP5 and HP5 + 2M glycerol), one kidney phantom (a low ionic strength gel), as well as rabbit kidney cortex have been measured from −10°C to −70°C.

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34

Bauer, M. L., C. M. Bauer, M. C. Fish, R. E. Matthews, G. T. Garner, A. W. Litchenberger, and P. M. Norris. "Thin-film aerogel thermal conductivity measurements via 3ω." Journal of Non-Crystalline Solids 357, no. 15 (July 2011): 2960–65. http://dx.doi.org/10.1016/j.jnoncrysol.2011.03.042.

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35

Çakıroğlu, Onur, Naveed Mehmood, Mert Miraç Çiçek, Aizimaiti Aikebaier, Hamid Reza Rasouli, Engin Durgun, and T. Serkan Kasırga. "Thermal conductivity measurements in nanosheets via bolometric effect." 2D Materials 7, no. 3 (May 1, 2020): 035003. http://dx.doi.org/10.1088/2053-1583/ab8048.

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36

Corradetti, S., M. Manzolaro, A. Andrighetto, P. Zanonato, and S. Tusseau-Nenez. "Thermal conductivity and emissivity measurements of uranium carbides." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 360 (October 2015): 46–53. http://dx.doi.org/10.1016/j.nimb.2015.07.128.

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37

Veiga, H. M. B., F. P. Fleming, and L. F. A. Azevedo. "Wax Deposit Thermal Conductivity Measurements under Flowing Conditions." Energy & Fuels 31, no. 11 (October 19, 2017): 11532–47. http://dx.doi.org/10.1021/acs.energyfuels.7b01131.

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38

Presley, Marsha A., and Philip R. Christensen. "Thermal conductivity measurements of particulate materials 2. Results." Journal of Geophysical Research: Planets 102, E3 (March 1, 1997): 6551–66. http://dx.doi.org/10.1029/96je03303.

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39

Cahill, David G., Henry E. Fischer, Tom Klitsner, E. T. Swartz, and R. O. Pohl. "Thermal conductivity of thin films: Measurements and understanding." Journal of Vacuum Science & Technology A: Vacuum, Surfaces, and Films 7, no. 3 (May 1989): 1259–66. http://dx.doi.org/10.1116/1.576265.

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40

Fahland, M., G. Mattausch, and E. Hegenbarth. "Thermal conductivity measurements on (Pb1-xBax)(Sc0.5Nb0.5)O3." Ferroelectrics 168, no. 1 (June 1995): 9–16. http://dx.doi.org/10.1080/00150199508007844.

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41

Doerk, Gregory S., Carlo Carraro, and Roya Maboudian. "Single Nanowire Thermal Conductivity Measurements by Raman Thermography." ACS Nano 4, no. 8 (July 22, 2010): 4908–14. http://dx.doi.org/10.1021/nn1012429.

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42

Chernodoubov, D. A., and A. V. Inyushkin. "Automatic thermal conductivity measurements with 3-omega technique." Review of Scientific Instruments 90, no. 2 (February 2019): 024904. http://dx.doi.org/10.1063/1.5084103.

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43

Kasubuchi, Tatsuaki. "Measurements of Thermal Conductivity and Diffusivity of Soil." Journal of Agricultural Meteorology 41, no. 1 (1985): 73–74. http://dx.doi.org/10.2480/agrmet.41.73.

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44

Dai, Sheng, Jong-Ho Cha, Eilis J. Rosenbaum, Wu Zhang, and Yongkoo Seol. "Thermal conductivity measurements in unsaturated hydrate-bearing sediments." Geophysical Research Letters 42, no. 15 (August 13, 2015): 6295–305. http://dx.doi.org/10.1002/2015gl064492.

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45

Jouglar, J., and P. L. Vuillermoz. "Dislocations in Plastically Deformed GaAs:Cr Thermal Conductivity Measurements." Materials Science Forum 10-12 (January 1986): 797–802. http://dx.doi.org/10.4028/www.scientific.net/msf.10-12.797.

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46

Lorenzini, M., E. Cesarini, G. Cagnoli, E. Campagna, K. Haughian, J. Hough, G. Losurdo, et al. "Silicate bonding properties: Investigation through thermal conductivity measurements." Journal of Physics: Conference Series 228 (May 1, 2010): 012019. http://dx.doi.org/10.1088/1742-6596/228/1/012019.

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47

HATTA, I., T. YAMANE, S. KATAYAMA, and M. TODOKI. "The Measurements of Thermal Conductivity of Carbon Fibers." Journal of Wide Bandgap Materials 7, no. 4 (April 1, 2000): 294–305. http://dx.doi.org/10.1106/qlxq-cadp-hc2m-f14u.

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48

McDowell, Matthew G., and Ian G. Hill. "Rapid thermal conductivity measurements for combinatorial thin films." Review of Scientific Instruments 84, no. 5 (May 2013): 053906. http://dx.doi.org/10.1063/1.4807898.

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49

Graves, R. S., D. W. Yarbrough, and D. L. Mcelroy. "Apparent Thermal Conductivity Measurements by an Unguarded Technique." Journal of Thermal Insulation 9, no. 2 (October 1985): 123–39. http://dx.doi.org/10.1177/109719638500900206.

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50

Allmaras, J. P., A. G. Kozorezov, A. D. Beyer, F. Marsili, R. M. Briggs, and M. D. Shaw. "Thin-Film Thermal Conductivity Measurements Using Superconducting Nanowires." Journal of Low Temperature Physics 193, no. 3-4 (July 24, 2018): 380–86. http://dx.doi.org/10.1007/s10909-018-2022-0.

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