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MICRF218 Datasheet(PDF) 15 Page - Micrel Semiconductor |
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MICRF218 Datasheet(HTML) 15 Page - Micrel Semiconductor |
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15 / 23 page ![]() Micrel MICRF218 November 2011 15 M9999-111111 (408) 944-0800 Table 3 shows the most used frequency values. Freq (MHz) C8 (pF) L1(nH) 315.0 6.8 39 390.0 6.8 24 418.0 6.0 24 433.92 5.6 24 Table 3. Band-Pass-Filter Front-End Values There is no need for the bandpass-filter front-end for applications where it is proven that the outside band noise does not cause a problem. The MICRF218 has image reject mixers which improve significantly the selectivity and rejection of outside band noise. Capacitor C3 and inductor L2 form the L-shape matching network. The capacitor provides additional attenuation for low frequency outside band noise, and the inductor provides additional ESD protection for the antenna pin. Two methods can be used to find these values, which are matched close to 50Ω. One method is done by calculating the values using the equations below, and the other method uses a Smith chart. The latter is made easier by using software that plots the values of the components C8 and L1, like WinSmith by Noble Publishing. To calculate the matching values, one needs to know the input impedance of the device. Table 4 4 shows the input impedance of the MICRF218 and suggested matching values for the most used frequencies. These suggested values may be different if the layout is not exactly the same as the one made here. Freq (MHz) C3 (pF) L2(nH) Z device (Ω) 315.0 1.5 68 16.3 -j210.8 390.0 1.2 47 8.26 – j163.9 418.0 1.2 43 11.1 – j161.9 433.92 1.1 39 9.54 – j152.3 Table 4. Matching values for the most used frequencies For the frequency of 433.92MHz, the input impedance is Z = 9.54 – j152.3Ω. The matching components are calculated by: Equivalent parallel = B = 1/Z = 0.410 + j6.54 msiemens Rp = 1 / Re (B); Xp = 1 / Im (B) Rp = 2.44kΩ; Xp = 345.8Ω Q = SQRT (Rp/50 + 1) Q = 7.06 Xm = Rp / Q Xm = 345.8Ω Resonance Method For L-shape Matching Network: Lc = Xp / (2×Pi×f); Lp = Xm / (2×Pi×f) L2 = (Lc×Lp) / (Lc + Lp); C3 = 1 / (2×Pi×f×Xm) L2 = 38.9nH C3 = 1.06pF Doing the same calculation example with the Smith Chart, it would appear as follows, First, the input impedance of the device is plotted, (Z = 9.54 – j152)Ω @ 433.92MHz.(Figure 8). Figure 8. Device’s Input Impedance, Z = 9.54-j152Ω Second, the shunt inductor (39nH) and the series capacitor (1.1pF) for the desired input impedance are plotted (Figure 9). One can see the matching leading to the center of the Smith Chart or close to 50Ω. |
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