Source: SCIENCE Volume: 297 Issue: 5590 Pages: 2229-2232 Published: SEP
27 ... Annex lead: Oak Ridge National Laboratory (H. Wang) .... Lab #1 P1-1.
Reliability of Transport Properties for Bulk Thermoelectrics Hsin Wang Oak Ridge National Laboratory Oak Ridge, TN USA
This project is supported by the International Energy Agency (IEA) under the Implementing Agreement on Advanced Materials for Transportation (AMT) 1
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Most Cited Thermoelectric Papers 1.
Title: Thin-film thermoelectric devices with high room-temperature figures of merit Author(s): Venkatasubramanian, R; Siivola, E; Colpitts, T; et al. Source: NATURE Volume: 413 Issue: 6856 Pages: 597602 Published: OCT 11 2001 Times Cited: 1,558
2.
Title: Large thermoelectric power in NaCo2O4 single crystals Author(s): Terasaki, I; Sasago, Y; Uchinokura, K, Source: PHYSICAL REVIEW B Volume: 56 Issue: 20 Pages: 12685-12687 Published: NOV 15 1997 Times Cited: 1,217
3.
EFFECT OF QUANTUM-WELL STRUCTURES ON THE THERMOELECTRIC FIGURE OF MERIT Author(s): HICKS, LD; DRESSELHAUS, MS Source: PHYSICAL REVIEW B Volume: 47 Issue: 19 Pages: 12727-12731 Published: MAY 15 1993 Times Cited: 1,017
4.
Quantum dot superlattice thermoelectric materials and devices Author(s): Harman, TC; Taylor, PJ; Walsh, MP; et al. Source: SCIENCE Volume: 297 Issue: 5590 Pages: 2229-2232 Published: SEP 27 2002 Times Cited: 925
5.
Title: Enhanced thermoelectric performance of rough silicon nanowires Author(s): Hochbaum, Allon I.; Chen, Renkun; Delgado, Raul Diaz; et al. Source: NATURE Volume: 451 Issue: 7175 Pages: 163-U5 Published: JAN 10 2008 Times Cited: 909
6.
Title: Cubic AgPbmSbTe2+m: Bulk thermoelectric materials with high figure of merit Author(s): Hsu, KF; Loo, S; Guo, F; et al. Source: SCIENCE Volume: 303 Issue: 5659 Pages: 818-821 Published: FEB 6 2004Times Cited: 905
7.
Title: Filled skutterudite antimonides: A new class of thermoelectric materials Author(s): Sales, BC; Mandrus, D; Williams, RK Source: SCIENCE Volume: 272 Issue: 5266 Pages: 1325-1328 Published: MAY 31 1996 Times Cited: 833
8.
Title: High-thermoelectric performance of nanostructured bismuth antimony telluride bulk alloys Author(s): Poudel, Bed; Hao, Qing; Ma, Yi; et al. Source: SCIENCE Volume: 320 Issue: 5876 Pages: 634-638 Published: MAY 2 2008 Times Cited: 617
9.
Title: Skutterudites: A phonon-glass-electron crystal approach to advanced thermoelectric energy conversion applications Author(s): Nolas, GS; Morelli, DT; Tritt, TM Source: ANNUAL REVIEW OF MATERIALS SCIENCE Volume: 29 Pages: 89-116 Published: 1999Times Cited: 287
10. Title: Properties of single crystalline semiconducting CoSb3 Author(s): Caillat, T; Borshchevsky, A; Fleurial, JP Source: JOURNAL OF APPLIED PHYSICS Volume: 80 Issue: 8 Pages: 4442-4449 Published: OCT 15 1996Times Cited: 271 2
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Mystery in Reporting Thermal Conductivity
ZT = s2σT/k k = αCpD
3
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Ref. #6
• Thermal conductivity is not measured • Thermal conductivity is calculated
Annex VIII Participants • IEA-AMT Thermoelectric Annex – Annex lead: Oak Ridge National Laboratory (H. Wang) – USA: Clemson (T. Tritt, S. Zhu); Marlow (J. Sharp); Corning (A. Mayolet, J. Senawiratne) and ZT-Plus (F. Harris) – China: SICCAS (S.Q. Bai, L. Chen) – Canada: Natural Resource Canada (J. Lo); University of Waterloo (Holger Kleinke); University of Quebec at Chicoutimi (Laszlo Kiss) – Germany: Fraunhofer IPM (H. Böttner, J. König )
• IEA-AMT members countries: – – – – – 4
UK: NPL Finland: VTT Israel: Australia: Republic of Korea: KERI (H. W. Lee)
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Marlow Materials Selected for Transport Properties Round-Robin Tests • Materials: Bi2Te3.005 (n-type) Bi0.5Sb1.5Te3 (p-type) • Four-sample Sets
– Thermal diffusivity: 12.7 mm diameter disk – Specific heat: 4 mm diameter disk – Seebeck coefficient and electrical resistivity: 2 x 2 x 15 mm3 bar, 3 x 3 x 12 m3 bar
• Temperature range: 300-500K • No ranking of the labs (lab numbers are assigned randomly in each plot)
5
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Round-robin 1: Thermal Diffusivity
n-type p-type
Results from 8 labs 6
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Round-robin 1: Seebeck Coefficient Lab #1 N 2x2
300
Lab #1 N 3x3 Lab #1 P 2x2 Lab #1 P 3x3 Lab #2 N 2x2 Lab #2 N 3x3 Lab #2 P 2x2
Seebeck Coefficient (µV/K)
200
Lab #2 P 3x3
p-type
Lab #3 N 2x2 Lab #3 N 3x3 Lab 33 P 2x2 Lab #3 P 3x3 Lab #4 N 2x2
100
Lab #4 N 3x3 Lab #4 P 2x2 Lab #4 P 3x3
2-point 0
Lab #5 N1 Lab #5 N2 Lab #5 P1
200
300
400
500
600
Lab #5 P2 Lab #6 N 2x2 Lab #6 N 3x3 Lab #6 P 2x2 Lab #6 P 3x3
-100
Lab #7 N 2x2 Lab #7 N 3x3
n-type
Lab #7 P 2x2 Lab #7 P 3x3 Marlow N Marlow P
-200
Lab #8 N 2x2 Lab #8 N 3x3 Lab #8 P 2x2
NIST SRM -300
7
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Lab #8 P 3x3 Lab #9 N 2x2 Lab #9 N 3x3
Temperature (K)
Lab #9 P 2x2 Lab #9 P 3x3 NIST SRM
Round-robin 1: Electrical Resistivity Lab #1 N 2x2
4.00
Lab #1 N 3x3 Lab #1 P 2x2 Lab #1 P 3x3 Lab #2 N 2x2
Electrical Resisivity (mOhm-cm)
3.50
Lab #2 N 3x3 Lab #2 P 2x2 Lab #2 P 3x3 Lab #3 N 2x2
3.00
Lab #3 N 3x3 Lab #3 P 2x2 Lab #3 P 3x3 Lab #4 N 2x2
2.50
Lab #4 N 3x3
n-type
Lab #4 P 2x2
2-point
2.00
Lab #4 P 3x3 Lab #5 N1 Lab #5 N2 Lab #5 P1 Lab #5 P2 Lab #6 N 2x2
1.50
Lab #6 N 3x3 Lab #6 P 2x2
p-type
1.00
Lab #6 P 3x3 Lab #7 N 2x2 Lab #7 N 3x3 Lab #7 P 2x2 Lab #7 P 3x3 Marlow N
0.50
Marlow P Lab #8 N 2x2 Lab #8 N 3x3
0.00
Lab #8 P 2x2
250
350
450
Temperature (K)
8
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550
Lab #8 P 3x3 Lan#9 N 2x2 Lab #9 N 3x3 Lab #9 P 2x2 Lab #9 3x3
Cp of Round-robin 1 with Debye Fit
p-type n-type
9
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Round-robin #2 Started in October 2010 • Procedures for DSC prepared by ORNL • Two sets of p-type samples – Set #1: ORNL -> Clemson-> Corning -> ZT-Plus -> Germany -> China -> Canada – Set #2: China -> (Japan) -> Germany -> ORNL -> Clemson-> Corning -> ZT-Plus -> Canada
• Completed in September 2011 • Report to IEA-AMT: October 2011 • IEA-AMT Topical report November 2011 10 Managed by UT-Battelle for the Department of Energy
Round-robin 2: Seebeck Coefficient 350
Seebeck Coefficient (µV/K)
300 250 200 150 100 50 0 250
300
350
400
Temperature (K)
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450
500
Lab #1 P1-1 Lab #1 P1-2 Lab #1 P2-1 Lab #1 P2-2 Lab #2 P1-1 Lab #2 P1-2 Lab #2 P2-1 Lab #2 P2-2 Lab #3 P1-1 Lab #3 P1-2 Lab #3 P2-1 Lab #3 P2-2 Lab #4 P1-1 Lab #4 P1-2 Lab #4 P2-1 Lab #4 P2-2 Lab #5 P1-1 Lab #5 P1-2 Lab #5 P2-1 Lab #5 P2-2 Lab #6 P1-1 Lab #6 P1-2 Lab #6 P2-1 Lab #6 P2-2 Lab #7 P1-1 Lab #7 P1-2 Lab #7 P2-1 Lab #7 P2-2 Marlow 2-point Contact
Round-robin 2: Electrical Resistivity 4
Resistivity (mOhm-cm)
3.5 3 2.5 2 1.5 1 0.5 0 250
300
350
400
Temperature (K)
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450
500
Lab #1 P1-1 Lab #1 P1-2 Lab #1 P2-1 Lab #1 P2-2 Lab #2 P1-1 Lab #2 P1-2 Lab #2 P2-1 Lab #2 P2-2 Lab #3 P1-1 Lab #3 P1-2 Lab #3 P2-1 Lab #3 P2-2 Lab #4 P1-1 Lav #4 P1-2 Lab #4 P2-1 Lab #4 P1-2 Lab #5 P1-1 Lab #5 P1-2 Lab #5 P2-1 Lab #5 P2-2 Lab #6 P1-1 Lab #6 P1-2 Lab #6 P2-1 Lab #6 P2-2 Lab #7 P1-1 Lab #7 P1-2 Lab #7 P2-1 Lab #7 P2-2 Marlow 2-point Contact
Round-robin 2: Thermal Diffusivity
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How Difficult is Thickness Measurement? α = 1.38d2/πt0.5
Thickness = 1.568 mm Thickness = 2.011 mm 14 Managed by UT-Battelle for the Department of Energy
Round-robin 2: Specific Heat
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Cp of Round-robin 2 with Debye Fit
16 Managed by UT-Battelle for the Department of Energy
Calculation of ZT: P-type
Calculated from Full Scatter • PF: + 7.1 to 11.7% • K: +8.5 to 17.9% • ZT: + 11.7 to 20.9% 17 Managed by UT-Battelle for the Department of Energy
Summary • Reliability of transport property is critical for vehicle applications • IEA-AMT is addressing this issue timely • Round-robin #3: 300K-800K – GMZ half-heusler materials for the round-robin effort (March 2012) – Materials processed and machined at GMZ Energy and first set measurements completed in May 2012
18 Managed by UT-Battelle for the Department of Energy