THHuxleynew , in this paper you can see the problems they are having are the inability to capture excess heat, not the contrary. This is a paper from the NEDO project updates by Akihito Takahashi, but they work in collaboration with Iwamura.
https://www.researchgate.net/p…E_Experiments_by_D-System
Thanks Curbina.
Are you sure that is the correct paper? Look at the abstract in italics at end of this post. Nowhere there do they mention problems disposing of excess heat. Rather, they say that they noted problems in their calorimetry of a low temperature system, and have therefore developed a system which will work at high temperatures (not - please note - larger amounts of excess heat).
Specifically they say low temperature work became inaccurate due to coolant boiling. But taht is only because they want to explore characteristics at higher temperatures.
It is understandable that therefore they move to a radiation-based heat transfer system.
Two TC sensors were added in the D-system, for monitoring gas temperature directly and RC center temperature. Variation of RC temperature distribution along the axial direction of RC cylinder in D-system became ca. 30 °C, which is less than 200 °C in the C-system runs 4-6). However, there remains considerable variation of temperature distribution in MHE sample zone for using three points average of sample TC temperatures to estimate excess power. We conceive that estimation of excess power by increment of H-gas temperature from calibration runs is most appropriate at the moment.
(PDF) New MHE Experiments by D-System. Available from: https://www.researchgate.net/p…E_Experiments_by_D-System [accessed Oct 01 2022].
So they have problems with varying temperature over the radiating surface and therefore can't do first principle calculation of enthalpy out. Instead they use comparison with a control.
My problem with that is that if the temperature distribution over the radiating surface is so uneven then it may differ between control and active, resulting in errors.
Time response of oil outlet temperature for removing heat by radiation transfer is found to be so slow (as more than 1 hour delay) that we cannot use for estimating time evolution of excess power generation. However, integral heat amount by oil mass flow is correctly estimated for very long time interval as several days. As a consequence, we decided to use excess power estimation by the H-gas temperature in RC for analysis of time evolution of excess power generation pattern, in correlation with dynamic evolution of H/Ni loading ratio1). We found that evolution of temperature at the mid-point of RC is most sensitive to the evolution of excess power generation. We can see rapid and clear AHE indication by this temperature evolution, but accurate estimation for excess power is difficult due to very local variation of AHE status.
(PDF) New MHE Experiments by D-System. Available from: https://www.researchgate.net/p…E_Experiments_by_D-System [accessed Oct 01 2022].
As I understand this they are not looking for integrated power out (for overall enthalpy) so all they get from the new system is the radiative info - which is inaccurate.
Since they say this I do not think we can take the system here as providing any evidence for excess heat in their system.
We have studied the so-called AHE (anomalous heat effect) by calorimetry of our C-system. The C-system was designed to make accurate detection of excess thermal power larger than several W/kg-sample. By our latest data with significant increase of excess thermal power of the MHE (nano-metal hydrogen energy) experiment, we have met to needs for improving the system. Especially in cases of observing 200W/kg-sample level excess power evolution using re-calcined PNZ-and CNZ-type MHE powder-samples, we have found some drawbacks in calorimetry with the C-system. We have therefore developed a new system, called D-system. In our new system (D-system), we have made the following improvements: a) Heat recovery system to cover higher temperature conditions as over 500°C of hydrogen gas condition of reaction chamber b) Increase detection points of heat sensors c) Reaction chamber assembly with high temperature-tight performance One drawback of the C-system was due to the problem that calorimetry inaccuracy became very large (underestimation) when coolant oil temperature reached at boiling point (ca. 350°C). In the D-system, we use the heat recovery by radiation heat transfer from the surface of reaction chamber settled in outer vacuum chamber. As a result, we can operate H-gas feeding runs with MHE sample powder to extend for much higher temperature conditions. We can take characteristic AHE data of excess thermal power with additional key data as evolution of H/Ni loading ratio. Characteristic feature of latest AHE data will be shown by another paper in this JCF22 meeting.