heat flow calorimeter
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2021 ◽  
Vol 2002 (1) ◽  
pp. 012007
Author(s):  
Xingye Wang ◽  
Bingjun Shen ◽  
Lihong Jin ◽  
Dan Zhou ◽  
Jian Tian

2020 ◽  
Vol 5 (8) ◽  
pp. 1410-1420 ◽  
Author(s):  
Manuel C. Maier ◽  
Michael Leitner ◽  
C. Oliver Kappe ◽  
Heidrun Gruber-Woelfler

The presented continuous flow calorimeter enables process understanding of novel flow syntheses and the use of highly reactive compounds. Adaptation of the calorimeter is possible via 3D printing and due to its modular and expandable design.


2016 ◽  
Vol 52 (5) ◽  
pp. 449-455 ◽  
Author(s):  
S. E. Mochalov ◽  
A. R. Nurgaliev ◽  
A. V. Antipin ◽  
E. V. Kuz’mina ◽  
V. S. Kolosnitsyn

2015 ◽  
Vol 25 (2) ◽  
pp. 45-52
Author(s):  
S. E. Mochalov ◽  
◽  
A. R. Nurgaliev ◽  
E. V. Kuzmina ◽  
V. S. Kolosnitsyn

2015 ◽  
Vol 1092-1093 ◽  
pp. 487-490
Author(s):  
Xing Ye Wang ◽  
Bing Jun Shen ◽  
Wu Shou Zhang ◽  
Li Hong Jin ◽  
Xin Lu ◽  
...  

Previously on the work [1-3] of excess heat triggering in a D/Pd gas-loading calorimeter system, we got that the system had the maximum excess power (6.398 ± 0.191 W) at the condition of an optimum current (8.47 A) and a deuterium pressure (3 × 104 Pa). In order to get higher excess heat power and to confirm the reliability and accuracy of the excess heat triggered by current in the previous work, we did a serials of experiments under different conditions. The results came from the heat-flow calorimeter system showed that the system produced the maximum excess heat power (10.284 ± 3.402 W) when the D2 pressure was 220 Pa. The key conditions of generating excess heat need to be further studied.


2014 ◽  
Vol 687-691 ◽  
pp. 874-877 ◽  
Author(s):  
Bing Jun Shen ◽  
Xing Ye Wang ◽  
Wu Shou Zhang ◽  
Li Hong Jin ◽  
Xin Le Zhao ◽  
...  

In order to confirm the reliability and accuracy of the excess heat triggered by current in the previous work [1-3], a new designed and built heat-flow calorimeter [4] was introduced in the same D/Pd gas-loading system as mentioned previously. The calorimeter was calibrated in nitrogen atmosphere and the results between the input power (P) and the exothermal electromotive force (V) could be simulated by a quadratic equation: P = (15.356 ± 0.068) V – (0.014 ± 0.039) V2. The maximum excess power (6.398 ± 0.191 W) were found at the condition of an optimum current (8.47 A) and a deuterium pressure (3 × 104 Pa). The reproducibility was 3/3 and the total excess energy released in these experiments was about 0.70 ± 0.02 MJ within 40 hours, which means (1.6 ± 0.1) ×103 eV for each palladium atom. The excess heat power and excess heat energy were far more than that in a chemical reaction.


2013 ◽  
Vol 102 (16) ◽  
pp. 163110 ◽  
Author(s):  
S. Sadat ◽  
E. Meyhofer ◽  
P. Reddy

2011 ◽  
Vol 110 (2) ◽  
pp. 1021-1027 ◽  
Author(s):  
Vratislav Tydlitát ◽  
Jan Zákoutský ◽  
Robert Černý

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