Description of the Related Art Transmission lines are used to connect various radio frequency circuit elements including connections from radio frequency (RF) circuits to antenna systems. Typical RF engineering practice dictates that a signal source should have an impedance equal to the impedance of the load. In addition, a load coupled to a transmission line should present an impedance equal to the characteristic impedance of the transmission line.

The importance of a matched load is that a transmission line terminated with a load equal to its characteristic impedance will transfer a signal without reflection.

In that instance, all power contained in the signal is transferred from the transmission line to the load. Loads with a resistance unequal to the characteristic transmission line impedance produce reflections.

Short sections of transmission lines can be used to tune a mismatched load by inserting the section across the conductors as a shunt, or in series with the mismatched line. The length of the transmission line, the type of termination, (open or shorted), and its location determine the effect on the circuit. At very short wavelengths, transmission lines function as circuit tuning elements.

One application of a matching network would be employed at the output of an RF signal amplifier. A typical push-pull RF amplifier output stage would require an output transformer with a center tap for carrying equal, direct currents through each half of the primary winding to the transistors. The secondary winding provides a balanced output at a different impedance for conversion to an unbalanced line and for further circuit connection. A matched load is therefore essential to maximize power transfer.

A balun (BALanced-UNbalanced) is a passive device which permits a transition between an unbalanced circuit and a balanced circuit and also permits impedance matching if necessary. The balun provides electrical isolation, but passes the transmission line currents. Baluns avoid the high frequency limitations of conventional magnetic transformers since the windings are arranged such that winding capacitance and inductance form a transmission line free of resonances.

Baluns can also provide impedance transformations with excellent broadband performance.

A prior art network converting a balanced output to an unbalanced output including an intermediate filtering network is disclosed in U. S. Patent Number

5,495,212. However, the intermediate filtering network revealed does not perform a tuning function for the equivalent circuit; the network provides low-pass filtering.

While the prior art has shown impedance matching transmission line transformers using a combination of eternal devices incorporating intermediate filtering, the conventional devices are overly complex when designed to operate over a wide RF bandwidth. What is needed is a balanced-to-unbalanced transmission line transformer that permits tuning of the overall frequency response characteristics of the circuit.

SUMMARY OF THE INVENTION The balanced-to-unbalanced broadband RF transmission line transformer of the present invention couples a twisted-wire transmission line between a center- tapped magnetic transformer and a balun. The location and function of the twisted- wire transmission line improves frequency response across a wide operational bandwidth by permitting the circuit to be tuned; thereby providing a greater degree of matching. The invention significantly improves frequency response over a 50- 860MHz operational bandwidth, while providing a conversion from a balanced to an unbalanced circuit with a high (4: 1) impedance ratio. The RF transformer exhibits a low voltage standing wave ratio (VSWR) with a minimal circuit burden.

Accordingly, it is an object of the present invention to provide a transmission line transformer that converts balanced inputs which are 180° out of phase with each

other to an unbalanced circuit while performing circuit tuning using a compensation transmission line to equalize the response characteristics over a large bandwidth.

Other objects and advantages will become apparent to those skilled in the art after reading the detailed description of a presently preferred embodiment.

BRIEF DESCRIPTION OF DRAWINGS Figure 1 is an electrical schematic of the preferred embodiment of the RF transformer.

Figure 2 is a perspective view of the magnetic transformer.

Figure 3 is a plot of the frequency response of the RF transformer over the operational bandwidth both with and without the compensation transmission line.

Figure 4 is a top view of the entire preferred embodiment.

Figure 5 is an alternative embodiment of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT The preferred embodiment will be described with reference to the drawing figures where like numerals represent like elements throughout.

Referring to the electrical schematic of Figure 1, the preferred embodiment of the RF transformer 17 is shown. The RF transformer 17 includes three discrete sections: 1) a center-tapped magnetic transformer 19; 2) atwisted-wire compensation transmission line 23; and 3) a balun 25.

The first section of the RF transformer 17 is a center-tapped magnetic transformer 19 with balanced primary input terminals 21 and secondary output nodes a and b. Nodes a and b are coupled to the second section, the twisted-wire compensation transmission line 23. The compensation transmission line 23 is shunted across nodes a and b and has a calculated variable characteristic impedance Zo and an electrical length. The output of the magnetic transformer 19, (nodes a and b), is also coupled to the third section, the 1: 1 balun 25. The balun 25 converts the balanced output a and b of the magnetic transformer 19 to an unbalanced RF output 27.

The physical construction of the magnetic transformer 19 and the balun 25 determines the characteristic inductance and capacitance of the RF transformer 17 and also determines the overall frequency response. The common mode inductance, or the primary inductance for a magnetic coupled transformer, determines the low frequency response of a transformer. Frequencies above the low frequency limit are coupled through the transformer core 39 and are unaffected by the common mode inductance. The high frequency limit is determined by transformer winding length and parasitic capacitance introduced by the common mode inductance.

In the preferred embodiment 17, the magnetic transformer 19 has a center- tapped primary 29 with five (5) turns and a balanced secondary 31 output having three (3) turns. A wire gauge of 36 AWG (American Wire Gauge) is used to form the primary 29 and secondary 31 around ferrite core 39. The input 21 is balanced across the primary positive 33 and negative 35 input terminals with the center tap

terminal 33 providing a common voltage supply for the balanced input 21. The input 21 is typically connected to a push-pull amplifier output stage (not shown).

The balun 25 is preferably wound with nine (9) turns of 3 8 AWG on a separate ferrite core 41. The output 27 of the balun 25 is unbalanced with a positive terminal 43 and a signal common (earthed) terminal 45.

The compensation transmission line 23 is constructed of twisted magnetic 36 AWG wire having a film insulation. As one skilled in this art would appreciate, the insulation may vary in thickness among four groups. A wide variety of characteristic impedances can be accomplished by varying the wire diameter, number of twists per inch, length, insulation film thickness and insulation film type. In the preferred embodiment, the compensation transmission line 23 is constructed of 36 AWG magnet wire, 0.5 inch in length, with sixteen (16) twists per inch.

The characteristic impedance, Zo, of the compensation transmission line 23 equals the ratio of voltage to current. The characteristic impedance of the preferred embodiment is 41Q. This characteristic impedance can also be expressed as the series wire inductance and inter-wire capacitance distributed along the length of the compensation transmission line 23. These relationships are well known to those skilled in the art of electronics. The result: Equation (1)

where Zo equals the characteristics impedance, L equals the parallel-wire inductance and Ct equal the total inter-wire capacitance.

As shown in Figure 2, the present invention 17 inside an amplifier preferably locates the compensation transmission line 23 within the ferrite core 39 of the magnetic transformer 19. The placement of the compensation transmission line 23 within the ferrite core 39 further provides a solid form around which to wrap the compensation transmission line 23 and keep it held in place. This ensures that the physical parameters of the compensation transmission line 23 will be the same for all manufactured units, and that the compensation transmission line 23 will not be inadvertently displaced once the RF transformer 17 leaves the manufacturing plant.

A plot of the frequency response of the RF transformer 17 inside an RF amplifier with and without the compensation transmission line 23 is shown in Figure 3. For the present invention, it was desired to limit the amplifier return loss to less than-18dB. The input RF signal is a sinusoid which sweeps over a 0-900 MHz bandwidth. As shown, the frequency response curve 60 for the RF transformer 17 without the compensation transmission line 23 exhibits a rise of over 5dB at 860 MHz. Accordingly, the return loss at 860 MHz is-13dB.

To equalize the response characteristics, the compensation transmission line 23 is inserted to tune the frequency response. The effect of the compensating transmission line 23 is shown by the frequency response curve 62 of Figure 3. The curve 62 shows a noticeable reduction in amplitude at 860 MHz and an overall flatter response across the design bandwidth of the RF amplifier. The use of the

compensation transmission line 23 clearly ensures that this return loss is kept below the-18dB reference line 64. It should be noted that the response characteristics shown in Figure 3 is representative of one embodiment tuned for a specific application.

Physical realization of the simplicity of the RF transformer 17 likewise is shown in Figure 4. The balun 25 is located adjacent to the magnetic transformer 19 upon a single substrate 50. This provides a compact and efficient utilization of space within a single package. The location of the compensation transmission line 23 is critical since improper placement may significantly degrade RF performance. The location of the compensation transmission line 23 is used to optimize the matching of the RF transformer 17 to an amplifier. Preferably, the compensation transmission line 23 is inserted through the core 39 of the magnetic transformer 19 and wrapped around a portion of the core 39, as shown in Figures 2 and 4. The compensation transmission line 23 could also be located around the periphery of the core 39 of the magnetic transformer 19. In this case, it would be preferable to include a groove (not shown) such that the compensation transmission line 23 is held securely in place.

It should be noted that alternative embodiments of the RF transformer 17 may use compensating transmission lines 23 constructed of coaxial cable. Additionally, physical construction of each transformer 19,25 may include toroids, rods, or symmetric cores of powered iron or ferrite. For example, as shown in Figure 5, a multi-hole (greater than 2) core 100 may be utilized to combine the transformer core 39 of the magnetic transformer 19 with the ferrite core 41 of the balun 25. This is particularly desirable for applications which require a compact design, since only a single core 100 is utilized.