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LTC5593 Datasheet(PDF) 16 Page - Linear Technology |
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LTC5593 Datasheet(HTML) 16 Page - Linear Technology |
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16 / 20 page ![]() LTC5592 16 5592f Values of L1A and L2A are tabulated in Figure 1 for vari- ous IF frequencies. The measured IF output return loss for bandpass IF matching is plotted in Figure 9. Table 3. IF Output Impedance vs Frequency FREQUENCY (MHz) DIFFERENTIAL OUTPUT IMPEDANCE (RIF || XIF (CIF)) 90 403 || – j610 (2.9pF) 140 384 || – j474 (2.4pF) 190 379 || – j381 (2.2pF) 240 380 || – j316 (2.1pF) 300 377 || – j253 (2.1pF) 380 376 || – j210 (2.0pF) 450 360 || – j177 (2.0pF) APPLICATIONS INFORMATION Figure 9. IF Output Return Loss with Bandpass Matching board (see Figure 2) has been laid out to accommodate this matching topology with only minor modifications. IF Amplifier Bias The IF amplifier delivers excellent performance with VCCIF = 3.3V, which allows a single supply to be used for VCC and VCCIF. At VCCIF = 3.3V, the RF input P1dB of the mixer is limited by the output voltage swing. For higher P1dB, in this case, resistor R2A (Figure 7) can be used to reduce the output impedance and thus the voltage swing, thus improving P1dB. The trade-off for improved P1dB will be lower conversion gain. With VCCIF increased to 5V the P1dB increases by over 3dB, at the expense of higher power consumption. Mixer P1dB performanceat1950MHzand2350MHzistabulatedinTable 4 for VCCIF values of 3.3V and 5V. For the highest conversion gain, high-Q wire-wound chip inductors are recommended for L1A and L2A. Low cost multilayer chip inductors may be substituted, with a slight reduction in conversion gain. Figure 10. IF Output with Lowpass Matching Figure 11. IF Output Return Loss with Lowpass Matching Lowpass IF Matching For IF frequencies below 90MHz, the inductance values become unreasonably high and the lowpass topology shown in Figure 10 is preferred. This topology also can provide improved RF to IF and LO to IF isolation. VCCIFA is supplied through the center tap of the 4:1 transformer. A lowpass impedance transformation is realized by shunt elements R2A and C9A (in parallel with the internal RIF and CIF), and series inductors L1A and L2A. Resistor R2A is used to reduce the IF output resistance for greater bandwidth, or it can be omitted for the highest conver- sion gain. The final impedance transformation to 50Ω is realized by transformer T1A. The measured return loss is shown in Figure 11 for different values of inductance (C9A = open). The case with 82nH inductors and a 1k load resistor (R2A) is also shown. The LTC5592 demo 4:1 T1A IFA 50Ω VCCIFA 3.1 TO 5.3V C5A 21 22 IFA– IFA+ C6 C9A R2A L1A L2A LTC5592 5592 F10 FREQUENCY (MHz) 50 –25 –20 –15 –10 0 –5 100 300 5592 F09 150 200 250 350 400 450 500 270nH 150nH 100nH 56nH 33nH 22nH –20 –25 –15 –10 0 –5 FREQUENCY (MHz) 50 0 100 150 5592 F11 200 250 68nH 100nH 180nH 82nH + 1k |
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