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DISCOVERY DSC 2090 DRIVER
However, as shown in Fig. Therefore, compared to the alloying discovery dsc 2090, the grain boundary scattering plays a secondary role in reducing the thermal conductivity of ZrCoBi-based materials. Therefore, in order to further minimize the lattice thermal conductivity, Sb alloying at the Bi site is conducted based upon the best composition of ZrCoBi 0.
As shown in the Supplementary Fig. In the meanwhile, the power factors of ZrCoBi 0.
To prove the reproducibility of the high performance of ZrCoBi 0. Detailed thermoelectric properties of the four samples are shown in the Supplementary Fig.
To further validate the high thermoelectric performance of ZrCoBi 0. The thermoelectric material will be referred as leg in the following was polished to the size of 1.
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The temperature of cold side was maintained by water circulation and temperature of hot side was controlled by PID. The direct measurement of Q in is of great challenge due to the heavy heat loss at discovery dsc 2090 temperature.
The thermal conductivity of the bulk polycrystalline graphite was confirmed before in the same way as described in the methods section. In order to measure discovery dsc 2090 differences of the leg and graphite bulk, K -type thermocouples were embedded at the interfaces. It should be noticed that the hot-side temperature of graphite can be regarded as the cold-side temperature of the leg if the setup is working under a large pressure as shown in Supplementary Fig. The total Q in includes Q outP and radiation loss from the leg Q rad. By tuning the current in the circuit, a series of Q in discovery dsc 2090, P can be measured at the same time.
To minimize the radiation loss, copper foil working as a radiation shield is brazed with copper plate of hot side. Since this radiation shield is at higher temperature than the leg, discovery dsc 2090 will add additional heat flow into the leg, therefore the measured Q out will actually be higher than without the shield.
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