Such sheet
metal shields, however, have low acoustical insulating value, and a large portion of
noise produced in an adjacent portion of an exhaust
system can be transmitted through the floor pan of the automobile and into the passenger compartment.
Additional
noise can be produced by loose shields which vibrate and / or rattle.
Where substantial acoustical shielding is also required,
metal shields, as described above, are not satisfactory.
However, such insulation can only be used where there are insignificant forces, both static and dynamic, on the fibrous insulation, since batts of fiberglass, for example, have very little strength in any direction, i.e. in either the X, Y or Z directions.
A very particular problem in regard to such shields has been encountered by the automobile industry and like industries, and that problem has become acute in recent years.
However, with modern designs, the spacing between the exhaust
system and the tunnel is now very much reduced, and in many situations, it is now no longer practical to suspend shields between the exhaust and tunnel, and, moreover, the reduced spacing correspondingly reduces any air gap remaining between the shield and the tunnel, such that very little conductive and convective heat insulation or acoustical insulation results.
The problem with such insulation is that the batts, especially of such inorganic fibers, are usually made by air laying fibers onto a moving belt, and, hence, the fibers tend to stratify in non-discrete
layers throughout the thickness (Z direction) of the batts.
However, because of the needling technique used in that process, the needle punch density could not be greater than about 260 needle punches per square inch, since, at above about 260 needle punches per square inch,
glass fiber damage resulted and with a more than 25% loss of mat strength.
While such an approach certainly improved Z-directional strength, with such low numbers of needle punches, the Z-directional strength of such a composite is still quite low and unacceptable for most modern thermal / acoustical insulating applications where substantial static and dynamic forces are placed on the insulation, e.g. in suspended use with an automobile, as discussed above.
However, shrinking fibers is not only a difficult process, but is substantially uncontrollable, and this approach does not result in uniform products.
Moreover, the tensile strengths, and particularly the Z-direction tensile strengths, are not greatly improved by that process.
While this approach is a very decided advance in the art, it still encounters difficulties when such batts experience high static and dynamic loadings, such as in the case of an automobile with a suspended shield, as described above.
However, the use of a
synthetic resin to achieve
formability of such a shield is a decided
disadvantage, since it is quite expensive to use a binder, and, moreover, the shield must be molded with conventional tools and dies, which themselves are quite expensive.
All of this is expensive and
time consuming in
assembly of the automobile and does not solve the problem or severely limited space in modern designs, as noted above.
However, with the combination of the protective foil, particularly when that foil is a
radiation barrier foil, and the composite batt, high
thermal insulation and high acoustical insulation results.
As can be appreciated, this results in a more expensive insulating shield, and in that sense, the arrangement for enclosing the insulating material is not as desired.