AVR2006: Design and characterization of the Radio Controller Board's 2.4GHz PCB Antenna. Application Note. Features.



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AVR26: Design and characterization of the Radio Controller Board's 2.4GHz PCB Antenna Features Radiation pattern Impedance measurements WIPL design files NEC model Application Note 1 Introduction This application note describes the PCB antenna used on the Radio Controller Board as a part of the ATAVRRZ2. This kit is designed for the evaluation of the Atmel AT86RF23 2.45 GHz radio transceiver. The radio transceiver fully complies with the IEEE 82.15.4 TM standard and targets low-power wireless technologies within homes, buildings and industrial automation such as ZigBee. Figure 1-1. ATAVRRZ2's radio controller board Rev. 895A-AVR-8/7

2 Antenna Design 2.1 Folded Dipole Considering a simple transmitting-receiving-system, the wireless transmission of signals requires the transformation of guided waves into spherical waves by use of an antenna. Therefore the antenna structure converts the guided wave into a propagated wave. The kind and manner of the radiation, depends strongly on the geometry and the environment of the antenna structure. It is essential to choose a design that allows matching either the antenna to the receiver, or to the generator for operation within a fixed frequency range, and to select the geometry for the required radiation. The designed antenna structure is similar to a dipole. A dipole is a symmetrical antenna of which both lines are being fed in the odd mode, meaning a phase shift of 18. The input impedance of an ideal dipole is approximately 73 ohm. In the case of one folding of the structure (creating a loop) the input impedance will be modified. The resulting value of the impedance is proportional to the square of the number of foldings used. Therefore a simple folded dipole has an impedance of 2 2 *73 ohm. If three lines were to fold to a λ/2 dipole, the impedance would change to 3 2 *73 ohm. As the realized antenna structure is being printed on a dielectric layer, the dielectric displacement currents flow between the lines and reduce the impedance considerably. Since the AT86RF23 datasheet states in section 3.5 that the AT86RF23 device has a differential impedance of 1 ohm at a frequency of 2.45GHz, it is now a matter of the geometrical dimensions to find values realizing a matching at the desired frequency. The properties of the antenna connection can be estimated by using electro magnetic (EM) field calculation software. Some programs like WIPL, Sonnet TM and Microwave Office allow simulating this structure on FR4 PCB material, other s such as the freeware application 4NEC2, only allow one to use free air as a dielectric. But experimenting with 4NEC2 can show the overall behaviour of geometrical changes, keeping in mind that the numerical solution will be wrong for FR4 or other PCB material. Figure 2-1. Folded dipole consisting of four lines. 2 AVR26 895A-AVR-8/7

AVR26 2.2 Board Antenna The finally realized antenna structure considers the symmetrical feeding, the influence of the substrate material, as well as the influence of the adjacent areas of ground on the circuit design. The boundary leading to the ground area should clearly be defined by using wire conductors (vias) between the top and the bottom metal layers. To interface a microstrip to a differential antenna structure, a Chip-Balun "WE- BAL 748421245" is used, allowing single ended measurements. This balun operates between 24MHz and 25MHz with an impedance ratio of 1:2. The balun's datasheet should be examined to find values for insertion loss and additional related parameters. The final antenna structure will be connected differentially to the RF port as demonstrated on the Radio Controller Board design. Figure 2.2 depicts the construction of the test board used during the measurements described in section 2.4 thru 2.7 of this application note. Figure 2-2. Test board. 3 895A-AVR-8/7

2.3 Mechanical Dimensions Figure 2-3. Test board. Table 2-3. Mechanical dimensions. Dimension [mm] [mil] x1 5.675 223.42 x2 5.179 23.9 x3 4.494 176.93 x4 3.452 135.9 x5 2.162 85.12 x6.738 29.5 x7 3.298 129.84 x8.3836 15.1 y 1.548 6.94 y1 5.675 223.43 y2 5.5 216.54 y3 4.933 194.21 y4 4.24 158.43 y5 2.845 112. y6 1.472 57.95 y7 1. 393.7 y8 5.659 222.79 w1 1.147 45.16 w2 1.411 55.55 w3.24 9.45 w4.311 11.85 4 AVR26 895A-AVR-8/7

AVR26 2.4 Port Impedance Figure 2.4-1 and 2.4-2 show the measured impedance of the antenna on the test board. The goal is it to reach a matching loss of db in the desired frequency band. The measured value at 2.45GHz is Z = 38 ohm / -15 so the antenna has an input impedance without balun of ZAntenna = 76 ohm, which creates a matching loss of.4 db. Reference plane for the following measurements is the SMA connector. Figure 2-4-1. Measured magnitude of port impedance. 1 9 8 7 magnitude (Z 11 ) mag (Z 11 ) [Ω] 6 5 4 3 2 1 2. 2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8 2.9 frequency [GHz] Figure 2-4-2. Measured phase of port impedance. 8 phase (Z 11 ) 6 4 phase (Z 11 ) [ ] 2-2 -4-6 -8 2. 2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8 2.9 frequency [GHz] 5 895A-AVR-8/7

2.5 Matching The impedance matching of this antenna is shown in figure 2.5. Between 2.4GHz and 2.5GHz the return loss is less than -1 db, which is equivalent to the behavior without a balun. The design goal here is it to reach an equal value of S11 than the generator delivers, which was reached here. Figure 2-4-3. Measured matching. -2 S11 [db] -4-6 S11 [db] -8-1 -12-14 1.6 1.8 2. 2.2 2.4 2.6 2.8 3. 3.2 3.4 frequency [GHz] 2.6 3D Radiation Pattern Figures 2.6, 2.7-1 and 2.7-2 show the radiation pattern in a spherical, horizontal and vertical view. The spherical view shows with the red intensity that the most intensive radiation direction is along the x-axis, with a direction gain of 6.5dBi and a 3dBbeamwidth of about 1. So the other communication end point should also be in that direction to make use of the antenna gain and prolong the transmission range. Figure 2-6-1. Calculated radiation pattern. 6 AVR26 895A-AVR-8/7

AVR26 2.7 Radiation Diagrams Figure 2-7-1. Measured horizontal radiation pattern. -5 12 9 6 horizontal radiation pattern -1-15 -2-25 15 3-3 -25-2 18-15 -1 21 33-5 24 27 3 Figure 2-7-2. Measured vertical radiation pattern. -5 12 9 6 vertical radiation pattern -1-15 -2-25 15 3-3 -25-2 18-15 -1 21 33-5 24 27 3 7 895A-AVR-8/7

2.8 Software The EM-field calculation software WIPL used in the design of this antenna can be found on http://www.wipl-d.com. The simulation files for this antenna can be found on www.atmel.com as "T3_WIPL.ZIP". Another EM-field calculator in the same league is Sonnet (http://www.sonnetusa.com/). Sonnet also offers a free version, which is limited to the calculated unknowns and PCB area. Those, who want to learn more about antenna simulation, may take a look at http://home.ict.nl/~arivoors/ to find the freeware 4NEC2. A geometrical model can be found on www.atmel.com as T3.NEC file. One should understand as a general note that the electromagnetic field solving software out in the market will never replace years of experience of antenna and PCB designers. It can only be a tool to calculate modeled behavior. The common antenna design process is a loop of creating and measuring an antenna object, since a lot of antenna properties cannot be modeled easily. Such properties are i.e. the antenna environment, distance to disturbing objects in the neighborhood and many more. All of those items may be add to the calculator's input, but it would take months to find results. So the appropriate tool concerning development time is it to include these parameters in the design loop for iterating and measuring parameters as shown in this document. 2.9 Gerber Files The Gerber files of this antenna and the Radio Controller Board can be found on www.atmel.com in the ATAVRRZ2 kit. 8 AVR26 895A-AVR-8/7

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