The way of attacking this problem is by considering the skirt as a unidimensional bar heated at one extremity, with constant cross section and infinite length.
Under such conditions the thermal flux (equivalent to what is calculated as
hA[Δ]
T elsewhere) is (from any heat transfer book):
q=
kAn[Δ]
T
where
k=thermal conductivity of skirt material
A=2[π]
Dt=cross section of skirt
D=skirt diameter
t=skirt thickness
[Δ]
T=temperature difference between vessel and ambient
n=[√](
hP/
kA)
P=4[π]
D=exposed perimeter (considering both faces of skirt as effectively exchanging)
h=heat exchange coefficient from skirt surface to ambient
The key factor is of course
h: this should account for a higher than ambient temperature at inside of skirt, and for any fireproofing or insulation covering the outer face (the initial portion of skirt covered by vessel insulation may be neglected, as essentially at uniform temperature).
I agree with the comments above that the heat loss through the skirt should be comparatively small if the skirt is fireproofed, however the length of the skirt plays a role in this case, and it all depends on what's considered as small by the owner...
prex
: Online tools for structural design
: Magnetic brakes for fun rides
: Air bearing pads