216
Chapter
4
8.3
Optimization
of
Plate Fin Exchangers and Constraints
on Weight Minimization
[SS]
Minimizing the material volume, or weight, of the plate-fin heat exchanger core does not
necessarily represents the optimum solution, even for weight-sensitive aerospace applications;
size and shape can be important design considerations
[a].
Minimum weight core could be
longer than is desirable because
of
the low fin efficiency implied. If the fin is too thin,
its
efficiency will be low, and to compensate both core length and flow area will be high, giving
an excessively high weight. On the other hand, a very thick fin giving high fin efficiency will
yield a low core length but with low porosity (free flow area) and weight. Minimizing the
components’ thickness can also contribute for low weight. But there are limitations in reducing
components beyond certain limits as follows:
The thicknesses of fin material and separating plates have lower limits set by pressure-retaining
capability.
Plate fin cores are usually made from sheet stock of a fixed range of thickness; rolling finstock
to a special “optimum” thickness could be uneconomic.
It may not be possible to form fins of sufficient dimensional accuracy if they are too thin;
if
they can
be
made, they might deform unsatisfactorily on brazing.
There may also be lower thickness limits set by erosion and corrosion problems.
9
EFFECT
OF
LONGITUDINAL HEAT CONDUCTION
ON THERMAL EFFECTIVENESS
The E-NTU and LMTD methods discussed are based on the idealization
of
zero longitudinal
heat conduction in the wall in the fluid flow direction. If a temperature gradient is established
in the wall in the fluid flow direction, heat transfer by conduction takes place from the hotter
to the colder region
of
the wall in the longitudinal direction. This longitudinal conduction in
the wall flattens the temperature distributions, reduces the mean outlet temperature
of
the cold
fluid, increases the mean outlet temperature of the hot fluid, and thus reduces the thermal
effectiveness
[63,65].
The reduction in the effectiveness at a specified
NTU
may be quite
significant for a compact exchanger designed for high thermal effectiveness (above
-80%)
and a short flow length,
L.
The shell and tube exchangers and plate exchangers
are
usually
designed for effectiveness of
60%
or less per pass. Therefore, the influence of heat conduction
in the wall in the flow direction is negligible for these effectiveness levels. The presence of
longitudinal heat conduction in the wall is incorporated into the thermal effectiveness formula
by an additional parameter,
h,
referred to as the longitudinal conduction parameter. Another
parameter that influences the longitudinal wall heat conduction is the convection conduction
ratio,
q@,
Thus, in the presence of longitudinal heat conduction in the wall, the exchanger
thermal effectiveness
is
expressed in a functional form
[65]:
9.1
Longitudinal Conduction Influence on Various
Flow
Arrangements
The influence
of
longitudinal conduction in the case of parallel flow is not discussed because
high-performance exchangers are not designed as for parallel flow arrangements. For high-
performance exchangers, the effect is discussed in Chapter
7,
Regenerators. In a crossflow
arrangement, the wall temperature distributions are different in the two perpendicular flow