Multiple pane glass unit with electrically conductive transparent film for use as radiation shield

1296573

MULTIPLE PANE GLASS UNIT WITH ELECTRICALLY CONDUCTIVE TRANSPARENT FILM FOR USE AS RADIATION SHIELD

This invention relates to a glass unit.

Our United States patent Number 4,721,636 issued January 26, 1988 relates to architectural windows to allow for good light transmission while shielding against radio frequency (RF) energy. The significance of RF shielding for architectural windows is directly associated with the dramatic growth and widespread use of radio frequency emitting devices. Radio stations, microwave relay stations, televisions, computers, two-way radios, and many other electronic devices either use or transmit electromagnetic energy in the radio frequency range - from 100 Hz to 100 GHz.

The need for shielding in buildings has several bases. One such basis is the protection of electronic equipment from interfacing with the operation of other electronic equipment. An example would be in the operation of high energy RF emitting equipment (e.g. a ship’s radar) which might penetrate a nearby building's outer shell and cause electronic error to occur in a digital computer system.

A second basis for shielding might involve the protection of people from RF energy, which in high doses causes tissues to heat, e.g. in the use of microwave ovens. In lower doses, other biological damage is possible.

A third need for shielding arises with concern for electronic spying - for political, economic or industrial advantage. This concern is justly based on the relative ease by which one can remotely (up to 2 miles away in some circumstances) monitor the information on a standard computer Cathode Ray Tube (CRT) screen.

The present application attempts to show a unique solution to the shielding of windows in buildings which require such protection. The above United States patent

<img file="CA1296579C_D0001.tif" />

expounded a concept which involved the use of a single transparent and electrically conductive film which was integrally mounted in a sealed insulating glass unit. Furthermore, a sin e, continuous wire cloth was used around the periphery, in direct contact with the electrically conductive film. This was accomplished by penetrating the seal of the glass unit without disrupting the hermetic quality of the unit.

The modifications and additions of the present invention involve essentially the same materials, however they are used in a way which offers shielding performance beyond that which would have otherwise been predicted. The use of multiple electrically conductive and transparent coatings (or films), which are produced by vacuum processes, (e.g. sputtering), creates and shield whose effectiveness exceeds the predicted results. These insulating glass unit so that to one another.

The invention is illustrated, the drawings, in which:

Fig. 1 shows a mult construction ;

Fig. 2 shows anothe of Fig. 1 ;

<td></td><td> Fig.</td><td> 3 is a graphic</td>

<td> tiveness</td><td> for a</td><td> film;</td>

<td></td><td> Fig.</td><td> 4 shows cavity</td>

<td> and</td><td></td><td></td>

<td></td><td> Fig.</td><td> 5 is a graphic</td>

<td colspan="2"> cavity width on</td><td> shielding.</td>

<td> Figure 1</td><td colspan="2"> illustrates the use</td>

<td> films in</td><td colspan="2"> conjunction with two</td>

films are assembled in the they are effectively parallel merely by way of example, in pie film and wire cloth version of the construction view showing shield effecwidth of the construction;

view showing the effect of f two conductive, transparent conductive, wire cloths.

This confirguration can also be utilized with a single wire cloth for grounding purposes, however, at a slight performance loss, as shown in Figure 2.

The performance of the single film/single cloth construction of the above United States patent application, showed experimentally to have a relatively flat shielding performance between 100 MHz and 10 GHz, ranging from 30-36 dB. This shielding performance can be predicted for this far field energy by the equation:

S^Edb = 20 log-jQ

<img file="CA1296579C_D0002.tif" />

(1) ^EEdb = Shielding Effectiveness in decibels

R = surface resistivity in ohms per square

Therefore, with a film that has R = 4 ohms per square, the predicted shielding effectiveness, SE^b» is equal to 33-5 db. This was verified through experimental measurement.

A means of predicting the shielding performance for multiple, parallel films is to consider an effective sheet resistivity based on a parallel resistor network.

_1_ = 1 + 1 ..... + 1 (2)

Reff Ri R₂ R_n

Where R_eff ₌ the effective sheet resistivity for n parallel films, ohms per square n = number of parallel films

Substituting into equation (1) results in:

<img file="CA1296579C_D0003.tif" />

(3)

<td> For two</td><td> films of</td><td> identical sheet</td><td colspan="2"> resistivity, equation (3)</td>

<td> reduces</td><td> to:</td><td></td><td></td><td></td>

<td></td><td>^SEdb ₌</td><td> 20 logqo 188 R</td><td> .5 + 6.02</td><td> (4)</td>

<td> Using R</td><td> = 4 ohms</td><td> per square for</td><td> both films,</td><td> results in:</td>

<td></td><td> SE_db -</td><td> 33-5 + 6.02 =</td><td> 39.52 db</td><td> (5)</td>

The conclusion is, therefore, that the addition of an identical, and parallel film will result in a theroretical maximum increase of 6 dB in the shielding effectiveness. Figure 3 illustrates that the additional benefit of two films, vs one film, approaches 6 dB as a maximum achievable benefit.

Actual test results on two film units found performance levels higher than the predicted value of 39 dB. Test samples made with a single ground cloth as illustrated in Figure 2, were found to have:

SE_db = 45 - 50 db (from 200 MH_Z - 1 GH_Z)

Test samples which utilized two films and two screens, Fig. 1, were measured to have:

SE_db = 55 - 60 db (from 200 MH_Z - 1 GH_Z)

These results show actual shielding performance to exceed predicted performance by 6 to 21 dB.

These unexpected benefits, it is beleived, can be explained by a more complicated model, whereby a cavity effect yields a greater than expected shielding performance. Through the numerical solution of Maxwell’s equations for plane waves, it is possible to predict not only these measured improvements, but to graphically illustrate the dependency on cavity dimension. This new approach for

<img file="CA1296579C_D0004.tif" />

modeling is based on optics (in the RF region of the electromagnetic spectrum) using multi-layer thin films, as opposed to the more convential analysis incorporating circuit modeling techniques. The optical model also allows for accurate prediction of single film shielding performance.

Through the use of this new modeling technique, it is possible to show the effects of cavity design on the performance of the shielding window. The main design criteria involves the distance separating the two conductive films; that is the width of the cavity. This is illustrated in Fig. 4.

By computing the shielding effectiveness as a function of frequency for various cavity widths, it is possible to see the dependency that performance has on this parameter.

This is shown for two conductive films (R = 2.2 ohms per square) in Fig. 5·

Given that the application of interst is for a sealed architectural window, the physical restrictions would limit the cavity widths to less than 4 cm. However, with specific design modifications, larger cavities can be made possible. It is predicted that at larger cavity widths, a resonance may occur which would significantly reduce the shielding at a particular frequency in the RF spectrum. If such a reduction in shielding occurred at an unwanted frequency, then the cavity width would have to be reduced.

It is clear from Fig. 5 that at all frequencies between 10 MHz and 10 GHz, the cavity design allows for equal or greater than expected results from previously held theories. These predictions have been experimentally verified. A shielding sample consisting of two films of 1.9 ohms per square were assembled as illustrated in Fig. 1.

1296573

This sample window measured 58 x 102 and was tested from 10 MHz to 1 GHx. The cavity width was 1.27 cm. Standard, theory would prdict from equation (1) and Figure (3) a shielding performance of 46 dB. Measured performance found an average attenuation greater than 50 dB, as well as a trend of improved performance with increasing frequency, as suggested in Fig. 5.

Accordingly, the present invention is an improvement in the prior single transparent, electrically conductive film, usd in conjunction with a single wire cloth ground. The present invention claims the addition of one more transparent, electrically conductive films and one or more wire cloth grounds. The performance of this multiple film/wire cloth product outperforms the expected (as predicted by conventional theory) shielding. A more extensive RF optical model does predict both the higher performance and the improved shielding at higher frequencies in the RF spectrum.