I'll try to better explain my position.
What I'm proposing is that mattwrigg's problem may be treated as a case of transient conduction in a one-dimensional slab.
This problem is solved in basic texts on heat transfer: an example is in section 5.3 of the Lienhard's free Heat Transfer Textbook that is the subject of a popular thread on this same forum.
The basic elementary treatment assumes a slab of sufficient extension in length and width so that in can be considered as infinite, and also with simmetry conditions through the thickness (both faces at the same temperature, mid plane with zero thermal flux across it).
Two simple boundary conditions may be treated analytically: faces at constant temperature and faces with convective heat transfer to a constant ambient temperature.
I think that the first one is closer to mattwrigg's conditions, as he regulates air temperature in order to maintain a constant slab face temperature of 55°C: the treatment of this one is also simpler, but also convection might be introduced for a closer approximation, especially during the first transient phase.
The solution is in series form, but the first term may be taken for a first approximation and is:
&[ignore]Theta[/ignore];=4/&[ignore]pi[/ignore]; x exp(-&[ignore]pi[/ignore];
2/4 x
&[ignore]alpha[/ignore];t/
L2)
where
&[ignore]Theta[/ignore];=(
T-
T1)/(
Ti-
T1)
T=temperature of mid plane as a function of time
T1=face temperature
Ti=initial temperature of slab
&[ignore]alpha[/ignore];=
k/
&[ignore]rho[/ignore];Cp
k=thermal conductivity
&[ignore]rho[/ignore];Cp=thermal capacity per unit volume
t=time
L=half slab thickness
Hence the time for reducing the temperature difference at mid plane with respect to faces by some 98% (but it's up to mattwrigg to define the functional goals) would be obtained from:
&[ignore]pi[/ignore];
2/4 x
&[ignore]alpha[/ignore];t/
L2=4
and
t&[ignore]asymp[/ignore];1.6
&[ignore]rho[/ignore];CpL2/
k
Now as my effort to arrive here has been quite important, I would like mattwrigg to fill in with some realistic values for
k and the other parameters to see what comes out.
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