For fusion, the activation energies are incredibly high. There is no way that the difference between 10C and 100C could be significant compared to the 10s of KeV required... However, because no-one has a credible mechanism for overcoming this activation energy <the authour?> is free to fit his ideas to whatever features he wants
I think it's a strange practice to fit ideas about plasma physics / collision fusion models into talking about LENR. It's clearly a MDOF many-body problem, with plenty of opportunities for emergent properties to arise. An example of one of these properties, is the Debye temperature.
The Slad paper... The hypothesis that LENR reaction rates depend on diffusion and so have linear temp dependence is OK. It has a glaring defect - why don't they happen at room temperature (which after all is itself a high temperature). Slad and others saying this need to propose some arbitrary and not understood cutoff which just coincidentally happens to be between room temperature and the higher operating temperatures used.
Yep, the Debye temperature: It's right there at the bottom of page 2. https://www.scribd.com/doc/283…g-Two-Chiefs-World-System
Worse, look at the graph in Slad's paper. Diffusion can only give dependence proportional to temperature in Kelvin (and similarly many other mechanisms). there is instead a linear graph proportional (roughly) to temperature above room temperature.
Ummm.. Debye temperature?? And you appeared to agree before that the 'linear' bit is not a completely crazy idea.
You do need some way maybe to heat your stuff up to get it started, under the assumption of the hypothesised unconvincing but convenient cut-off to linear temperature dependence.
Nice way to build an entire argument around a red herring. I don't think the Debye temperature is an "unconvincing" thing to toss in there... It tells us the temperature at which peak phonon (lattice) pressure stops occuring only at the outside face of the metal lattice, and starts sweeping periodically throughout the entire crystal structure.
The idea of the Debye temperature being some kind of ignition point comes from two of Piantelli's patents. It should also be noted that in the Storms paper that I reference, he first sees a noticeable excess heat signal at about 30C above the Debye temperature of Pd. Interestingly, this is just slightly above room temperature.
The idea that the best way to control a linear with temperature exothermic reaction is variable input heat...
This is ludicrous. You have a very limited range of adjustment - if you have COP = N then you can accommodate at most 1/N variation in reaction rate due to random factors.
I agree up to a point. What you say is obviously correct, if you consider the reactor as a steady-state device. A COP of around 8-10 is probably a reasonable limit, for the reasons you suggest.
LENR is clearly (if it exists) variable and so to make it safe you need a control system that could stabilise temperature over a wide range of powers. That is an output side (cooling) system. It is easy to make such systems which are highly effective and temperature controlled. They can easily stabilise power variations of 10X in the reaction rate.
There are few benefits, and several problems, offered by the type of system you propose:
1. To allow stable and efficient heat transfer, the reactor must have some sort of thermal resistance between the fuel and the cooling water (The Leidenfrost effect is an extreme example of why this is). This buffer will also have a thermal capacitance.
2. High thermal capacitance is a good thing, with controlled heating, if you consider the heat flow in the time-domain, it becomes apparent that in some cases ** including those with an exponential fuel-power curve ** the COP can be increased beyond 8-10 by causing the fuel to oscillate between two temperatures*. Essentially you are letting the fuel heat itself up, before the rate of heat transfer rises enough to cool it. Tight control is needed. These ideas are discussed with Dave Roberson in more detail here: https://disqus.com/home/discus…enwin/#comment-2318439426
3. In your case, you are trying to control fuel temperature, but your control input is on the wrong side of the thermal capacitance. This is refered to in my comment about "reset-time" on page 5 of my report. The reality is you would have to dramatically slow down the response of your pump, in order to stop it fluctuating wildly between on and off states. It is also possible you could decrease the pumps responsiveness so much, it would be unable to control a fuel with a 'peaky' power curve. Or even any fuel at high COPs.
4. I agree that some form of negative feedback in the cooling system is of great benefit. Fortunately, we don't need your proposed metered cooling system for this to happen: Water already has this property. Basically it's heat transfer coefficient significantly increases proportionally to its rate of boiling (up to a critical temperature). This effect is driven by different bubble formation regimes appearing, the differences between which can no doubt be heard by a stethoscope...
5. With a metered cooling system, as you propose, where does the increased amount of 'returned' hot water go? It's a waste to pour it down the drain, and it can't easily be fed back into the cold water input. One solution is an additional heat exchanger, and drain it (although this still would present some problems), the other solution is a closed-loop primary cooling circuit, more akin to a nuclear power plant, which would require both an additional heat exchanger and an additional pump.
6. This isn't some large nuclear power plant. It's distributed power. Installations need to be as simple as possible, both to keep down manufacturing costs, and reduce maintenance hours.
7. Metered cooling treats the whole heat exchange surface as a single element, with controlled heating, separate bands can be heated independently, to smooth the power delivery or temperature, at all points along the path of water flow.
* As you say, this would perhaps involve finding a stable region of the operating envelope where fluctuations due to "random factors" are not a problem