Background of the Invention
1. Field of the Invention
This invention relates to a windowpane or windshield antenna, having a thin, electrically conductive layer flatly applied to an area of the windowpane, which is transparent to light, but reduces the transmission of heat.
In the invention, the conductive area is mounted on the windowpane, and is either directly applied to the window glass, or embedded between two layers of glass to form a composite or safety glass pane. A thin foil may serve as carrier of the conductive layer. This foil may be embedded between the glass panels of the composite or safety glass pane. When this layer is used as the main element of an antenna, it is desirable to use layers with the lowest possible surface resistivity. The lower the surface resistivity of the conductive areas formed by extremely thin metal and metal oxide layers, the higher the light-absorbing effect in the visible area. However, conductive layers with sufficiently high transparency cannot be realized with a surface resistivity of highly conductive materials such as copper or silver. These materials have a surface resistivity around 0.25 milliohm, which is lower by many orders of magnitude.
2. The Prior Art
Antennas of this type are preferably used in motor vehicle windshields where the conductive layer should be kept as transparent as possible. For this reason, the surface resistivity of the conductive layer must not be below 5 ohms. Antennas of this type are preferably used as radio reception antennas in the long, medium and short wave, VHF and UHF frequency ranges.
German Patent No. 37 21 934 A1 describes an antenna which uses a relatively low-resistive conductive layer. However, if antennas of the prior art are designed with layers of higher resistivity with better transparency, the antenna losses are relatively high, which results in comparatively low antenna capability. Such antenna losses have highly adverse effects, especially in the meter and decimeter (VHF) ranges.
Summary of the Invention
It is therefore an object of the present invention to provide a windshield antenna, which avoids the loss of capacitance caused by limited conductivity in its conductive area.
Antennas according to the prior art have point-like contacts for connecting them to the area of limited conductivity formed by the conductive layer. High antenna current densities are thus produced within the zone of these contacts. These current densities contribute substantially to the antenna losses on the glass surface due to limited conductivity. The antenna according to the invention avoids this drawback through a suitable embodiment of a connection electrode.
The present invention provides an antenna for a windowpane or windshield, comprising a thin, electrically conductive layer flatly applied to an area of the window. The layer is transparent to light, is capable of reducing the transmission of heat through the windowpane, and creates a low-conductive area having non-negligible surface resistivity on the windowpane. Also provided is a substantially flat electrode made of highly conductive material, which is high-frequency connected with a reduced high-frequency loss at at least one edge to the low-conductive area, and also high frequency connected to an antenna connection point. The electrode has a length sufficiently large so as to minimize the loss created by the edge of the low-conductive area.
Brief Description of the Drawings
Other objects and features of the present invention will become apparent from the following detailed description considered in connection with the accompanying drawings. It is to be understood, however, that the drawings are designed as an illustration only and not as a definition of the limits of the invention.
In the drawings, wherein similar reference characters denote similar elements throughout the several views:
FIG. 1a shows an antenna according to the invention having an area with limited conductivity disposed on a windowpane with an elongated electrode made of highly conductive material;
FIG. 1b shows the mode of operation of an antenna electrode according to the invention, with distributed current lines as shown, for avoiding current concentrations over a larger area with limited conductivity;
FIG. 1c shows a low conductive area and point-like contact according to the state of the art, showing current line concentrations near the point-like contact, and showing an area of particularly high contribution to loss by the dashed line;
FIG. 2a shows a composite glass pane with an embedded low-conductive area, and having capacitively coupled electrode on one of its outer glass surfaces, with an antenna connection point;
FIG. 2b shows an electrode as in FIG. 2a, but with a meandering inductance for partly compensating for the capacitive reactance within a limited reception frequency range;
FIG. 2c shows electrode with capacitive coupling as in FIG. 2b, with inductors with a selectable antenna connection point on the electrode;
FIG. 3 shows a motor vehicle antenna according to the invention in the front windshield, with a strip-like electrode of a defined electrode length and width;
FIG. 4 shows an antenna in the front windshield of a motor vehicle, with strip-like electrode serving as a frame for the entire window opening;
FIG. 5a shows a radio reception antenna system on a windshield with three separate antennas for ultra-short wave diversity, and the effective areas of the individual antennas are defined by the dashed lines;
FIG. 5b shows a composite or safety glass pane with a low conductive embedded area, with an additional electrode capacitively coupled in a thin plastic sheet; and
FIG. 5c shows a composite glass pane wherein an additional electrode rests directly on a low conductive area so that a galvanic contact is established.
Detailed Description of the Preferred Embodiment
Referring to FIG. 1a, there is shown an antenna having an elongated electrode 6 made of highly conductive material having an electrode length 5, a width 9, and an antenna connection point 8. A coax cable having a grounded shield 3 connects to point 8. Along the margins, high frequency contact is established with a low-conductive area 4, which prevents any concentration of current. This is shown in FIG. 1b, where the indicated current lines show that the total current 1 supplied to electrode 6 via the connection point 8 is almost uniformly distributed via the highly conductive electrode 6 and admitted into low-conductive area 4, thus avoiding high current densities. In contrast to the above, a point-like connection such as the one in FIG. 1c, shows high current densities within the vicinity of the point-like connection, thus causing high contribution to loss from the proximity of the connection as defined by the dashed line.
It has been confirmed in empirical tests that when an ultra-short wave antenna is designed as shown in FIG. 3, the optimal design length 5 of electrode 6 is approximately 30 cm or 12 inches. Width 9 of electrode 6, which is galvanically connected to low-conductivity window 4 in the present case, can be varied within wide limits. However, this width should not be excessively small, so that its own inductance will be too low. An electrode width 9 of about 5 mm has been found to be suitable. When designing motor vehicle antennas, it is always necessary to take into account that the electrodes, for aesthetic reasons, should be covered by the black print usually located along the edge of the pane. This means that the low-conductive area should be designed so that it covers the entire range of sight, and ends within the back print, where it is contacted by the electrode.
Preferably, the space between the edge of low-conductive area 4 and the conductive window frame 2 should be made as large as possible. Because of the limited width of the black print, the width 9 of electrode 6 should be as large as electrically required for coupling with low-conductive area 4, but not excessively large in order to maintain the largest possible spacing from the conductive window frame 2. An antenna such as the one shown in FIG. 3 can be used for a long, medium and short wave signals, as long as low-conductive window area 4 is not at any point galvanically or capacitively connected to conductive window frame 2 with excessively low resistivity. Therefore, low-conductive area 4 coupled to electrode 6 according to the invention can also be designed as a long, medium and short wave antenna, allowing it to be used for television and audio reception.
According to a particularly advantageous embodiment of the invention, electrode 6 can be designed in the form of a frame, as shown in FIG. 4. This avoids particularly high losses, especially when layers are used with higher resistivity than low-conductive area 4.
The limited conductivity of layer 4 can be used to form individual antennas that are partly decoupled from each other. As shown in FIG. 5a, antennas are formed so they are separated from one another. The main field of activity of each antenna is defined by the dashed line. For ultra-short wave application, electrodes 6 each have a length of approximately 30 cm. The diversity effect results from the distribution of electrodes 6 over the circumference of the conductive window frame 2a, 2b and 2c. It was found that decoupling near the lower horizontal part 2c of the window frame preferably absorbs the vertical components of the electrical field. Antennas near the upper horizontal part 2a and close to the vertical struts 2b preferably absorbs the horizontal components of the electrical field. The individual antennas FM 1/AM, FM2, FM3, and FM4 are capacitively coupled to an antenna switch 50, which is in turn connected to AM and FM receivers. Thus, an effective diversity reception installation can be formed with the antenna system shown in FIG. 5a.
The decoupling of long, medium and short wave signals can take place on one of the antennas. However, effective antenna loads in the long, medium and short wave ranges must be kept as low as possible by loading the low-conductive area 4 using the ultra-short wave connections of the diversity system. This is accomplished by capacitors 10 as shown in FIG. 5a, connecting the diversity system to the antennas. Their capacitance value must be sufficiently high so as to provide an adequately low reactance for the higher frequencies. However, the sum of capacitors capacitively loads area 4 for the long, medium and short wave frequency ranges and reduces the LMS or AM-signal. Within a limited frequency range, such as for example in the ultra-short wave range, it is possible to partially compensate for the capacitive reactance by using a series-connected inductance, so that lower capacitive values can be used.
Capacitive coupling with low conductive layer 4 can be accomplished by embedding the layer between the panes of the composite glass, and printing a strip-like electrode 16 into the side of the composite glass facing the interior of the vehicle, and then coupling the electrode to this area as shown in FIGS. 2a, 2b or 2c.
In FIG. 2b, an inductor 17 is provided for partly compensating for the capacitive reactance of capacitor 10 and can be printed onto the surface of the glass as well. This can be done as shown in FIG. 2b by providing the inductor at one end of electrode 16.
As shown in FIG. 2c, electrode 26 is divided so as to provide an inductor 27 in the middle portion. Thus, it is possible to fine tune the antenna by selecting a connection point 8 along the length of inductor 27 to compensate for the capacitance of the circuit.
FIG. 5b shows a composite glass pane with a low-conductive embedded area 4, and an additional electrode 36a added thereto. Electrode 36a is capacitively coupled via a thin plastic sheet 11, or galvanically coupled with an additional electrode 36a on one of the outer surfaces of the glass opposite the conductive surface for forming the electrode 6 consisting of a conductive area having substantially the same form as additional electrode 36a.
According to another embodiment of the invention, it is possible to further reduce the remaining coupling losses by providing an electrode 16 as shown in FIG. 2a or 2b on one of the outer surfaces of a composite glass windowpane with capacitive coupling to low-conductive area 4. Moreover, losses can also be reduced when an additional electrode, such as electrode 36a is provided in the embodiment of FIG. 5b. Electrode 36a adjoins the glass composite, or is mounted on an inner surface of the glass opposite electrode 36 for the purpose of forming a capacitor. Advantageously, additional electrode 36a is designed in the form of a conductive area having substantially the same contour as electrode 36. As seen in FIG. 5b, a thin foil may be present between additional electrode 36a and low-conductive area 4. This foil should not noticeably reduce the effective capacitance between additional electrode 36a and electrode 36. It is, therefore, particularly advantageous if, as shown in FIG. 5c, an additional electrode 46a rests directly on low-conductive area 4, opposite electrode 46, so that a galvanic contact is established.
Accordingly, while several embodiments of the present invention have been shown and described, it is obvious that many changes and modifications may be made thereunto without departing from the spirit and scope of the invention according to the appended claims.