2015
DOI: 10.7567/jjap.54.026602
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Simultaneous measurement of the Seebeck coefficient and thermal diffusivity for bulk thermoelectric materials

Abstract: We simultaneously measured the Seebeck coefficient and thermal diffusivity of a rectangular parallelepiped bulk thermoelectric material. We used one-dimensional heat conduction equation to show that a periodic heat cycle produces not only the thermoelectromotive force but also a certain phase shift angle between the edge and intermediate points of a sample along the length of the material. Based on the equation of the modified Angström method, an experiment at 300 K was performed using NIST standard material (… Show more

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Cited by 11 publications
(12 citation statements)
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“…3 shows the temperature dependence of the assumed Seebeck coefficient from 25 K to 300 K from previous work as a conditional value. 14,20 By the definition of zT, it also shows the estimated temperature dependence of the thermal conductivity for the module (κ = S 2 ρzT T ). At 300 K, the estimated thermal conductivity was ∼1.90 W/mK, which is reasonable compared to that for the NIST Bi 2 Te 3 sample (measured to be 2.06 W/mK by the steady-state method at 300 K in a previous study).…”
Section: Resultsmentioning
confidence: 99%
“…3 shows the temperature dependence of the assumed Seebeck coefficient from 25 K to 300 K from previous work as a conditional value. 14,20 By the definition of zT, it also shows the estimated temperature dependence of the thermal conductivity for the module (κ = S 2 ρzT T ). At 300 K, the estimated thermal conductivity was ∼1.90 W/mK, which is reasonable compared to that for the NIST Bi 2 Te 3 sample (measured to be 2.06 W/mK by the steady-state method at 300 K in a previous study).…”
Section: Resultsmentioning
confidence: 99%
“…Thermal conductivity was derived from κ = ρ DC p , where ρ is density of the sample, and C p is heat capacity measured by differential scanning calorimetry. The thermal diffusivity was measured under a vacuum (<5 × 10 –3 Pa) by a modified Ångström method with the same experimental configuration in the measurements of Seebeck coefficient and electrical conductivity. A sinusoidal current was supplied to the heater for creating a periodic heating wave at frequency of 0.01–0.02 Hz via Joule heating.…”
Section: Methodsmentioning
confidence: 99%
“…[11][12][13][14][15][16][17][18][19] We also proposed a modified Angström method of estimating the thermal diffusivity by detecting the thermoelectric voltage directly on an element without thermosensors. 20) In addition, the method has been extended to measure not only the thermal diffusivity α but also the Seebeck coefficient S, resistivity η, thermal conductivity λ, and heat capacity C, as well as the figure of merit, using an identical thermoelectric element. 21) However, this technique cannot be applied to much shorter thermoelectric elements, especially the elements in a typical module, because their usual length is less than 2 mm, and it is difficult to attach local electrodes on the side surface of elements in the module using Ag epoxy.…”
Section: Introductionmentioning
confidence: 99%
“…Here, we note that the thermal diffusivity of thermoelectric materials was predicted to be on the order of 10 −6 m 2 =s. [19][20][21] The required periodic frequency of the heat is estimated as 0.22 Hz when the length of the element is 1 mm, the phase shift angle is 10°, and a measurement point at the midpoint of the sample is used. 20) This means that the thermal diffusivity on the module can be estimated if the temperature is measured using real-time acquisition without any contact with an infrared (IR) camera in a so-called thermographic method.…”
Section: Introductionmentioning
confidence: 99%