The other day it was proposed (Lennart Thornros) that a small steel plate could 
be placed above an induction heating stove top to intercept a significant 
quantity of magnetic flux for fuel heating.   I decided to make a quick 
estimate of the power required if this were to be used to raise the plate 
temperature to 1200 C(1474.15 K).

My preference is to continue the experimental designs using a heating element 
consisting of high temperature wires.  They allow the experimenter to measure 
the input power much easier than induction techniques.  They are also smaller 
and less expensive.  But, in the interest of science it is important to keep an 
open mind as far as possible hence this discussion.

I chose a rough surface steel plate that is 5 cm by 5 cm by .2 cm and assumed 
it is lying flat upon the induction coil.  The only path I calculated for the 
escape of heat is by radiation.  Any additional convection or conduction would 
increase the total power required.  There are 6 total radiating areas in this 
assumed structure with a total area of .0054 square meters.  I used an 
emissivity of .45, which may need some adjusting at the operational temperature.

Using Boltzmann's constant of 5.67*10^-8 I arrived at a power requirement of 
651 watts.  The formula is P=.45 x .0054 x 5.67 * 10^-8 x 1474.15 ^4.  This 
level of power is within the ratings of a typical induction heating element 
provided that the steel plate intercepts a sufficient amount of magnetic flux.  
If a larger steel surface area is required, then the power goes up in direct 
proportion to the area increase.

I read the specifications of some of these inexpensive devices and they appear 
to make a determination that there is a sufficient load before attempting to 
apply power into it.  This of course will set limits upon the size and type of 
material used to heat the fuel.  And, if the steel plate is raised above the 
element surface less magnetic flux will be encountered and thus a larger plate 
may be needed.  Most of the water calorimeters along with some type of 
interface between the steel plate and the water take vertical space.

With these requirements in mind I picture a relatively small(5x5x.5 (cm)) 
milled out block of steel having a cavity just large enough to hold the fuel 
plus any required extra room.  A carefully cut piece of ICE high temperature 
head gasket material can be used as a seal between the lower milled out steel 
block and a steel cover that is screwed on.  This should yield an air tight 
design but I am confident that hydrogen will escape easily given enough time.  
At least this should keep water vapor from getting to the fuel.

I have not come up with a good method of interfacing the steel fuel chamber to 
the water bath of the calorimeter.  The outer surface of that interface box(?) 
is at 100 C while it receives radiation from the steel chamber being held 
within it.  Parkhomov used a steel pot to make the transition.  In our case the 
material needs to be transparent to changing magnetic flux(alumina?).

Take this posting as just a beginning concept so please add your ideas.  I can 
see that it is going to be a challenge to get all the pieces to work together 
with this type of system, but challenges are what makes life interesting.

Dave

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