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AD8362 Datasheet(PDF) 24 Page - Analog Devices |
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AD8362 Datasheet(HTML) 24 Page - Analog Devices |
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24 / 32 page ![]() AD8362 Data Sheet Rev. E | Page 24 of 32 TEMPERATURE COMPENSATION AT VARIOUS WiMAX FREQUENCIES UP TO 3.8 GHz The AD8362 is ideally suited for measuring WiMAX type signals because crest factor changes in the modulation scheme have very little affect on the accuracy of the measurement. However, at higher frequencies, the AD8362 drifts more over temperature often making temperature compensation necessary. Temperature compensation is possible because the part-to-part variation over temperature is small, and temperature change only causes a shift in the AD8362’s intercept. Typically, users choose to compensate for temperature changes digitally. How- ever, temperature compensation is possible using an analog temperature sensor. Because the drift of the output voltage is due mainly to intercept shift, the whole transfer function tends to drop with increasing temperature, while the slope remains quite stable. This makes the temperature drift independent of input level. Compensating the drift based on a particular input level (for example, −15 dBm), holds up well over the dynamic range. Figure 59 through Figure 63 show these results. The compensa- tion is simple and relies on the TMP36 precision temperature sensor driving one side of the resistor divider as the AD8362 drives the other side. The output is at the junction of the two resistors (see Figure 58). At 25°C, TMP36 has an output voltage of 750 mV and a temperature coefficient of 10 mV/°C. As the temperature increases, the voltage from the AD8362 drops and the voltage from the TMP36 rises. R1 and R2 are chosen so the voltage at the center of the resistor divider remains steady over temperature. In practice, R2 is much larger than R1 so that the output voltage from the circuit is close to the voltage of the VOUT pin. The resistor ratio R2/R1 is determined by the temperature drift of the AD8362 at the frequency of interest. To calculate the values of R1 and R2, first calculate the drift at a particular input level, −15 dBm in this case. To do this, calculate the average drift over the temperature range from 25°C to 85°C. Using the following equation, the average drift in dB/°C is obtained. e Temperatur Error Δ dB C dB/ = ° (16) In this example, the drift of the AD8362 from 25°C to 85°C is −2.07 dB and the temperature delta is 60°C, which results in −0.0345 dB/°C drift. This temperature drift in dB/°C is con- verted to mV/°C through multiplication by the logarithmic slope (51 mV/dB at 2350 MHz). The result is −1.76 mV/°C. The following equation calculates the values of R1 and R2: C) (mV/ C mV/ 10 ° ° = Drift AD8362 R1 R2 (17) Table 5 shows the resultant values for R2 and R1 for frequen- cies ranging from 2350 MHz to 3650 MHz. Figure 59 through Figure 63 show the performance over temperature for the AD8362 with temperature compensation at frequencies across the WiMAX band. The compensation factor chosen optimizes temperature drift in the 25°C to 85°C range. This can be altered depending on the temperature requirements for the application. Table 5. Recommended Resistor Values for Temperature Compensation at Various Frequencies Freq. (MHz) Average Drift @ −15 dBm (dB/°C) Slope (mV/dB) Average Drift @ −15 dBm (mV/°C) R1 (kΩ) R2 (kΩ) 2350 −0.0345 51 −1.7600 4.99 28 2600 −0.0440 51.45 −2.2639 4.99 22.1 2800 −0.0486 51.68 −2.5102 4.99 20 3450 −0.0531 51.61 −2.7402 4.99 18.2 3650 −0.0571 51.73 −2.9544 4.99 16.9 INHI INLO CLPF VSET VOUT VOUT 0.1µF VTGT VREF 0.1µF R1 R2 5V AD8362 1nF 2.7nH 4.7nH 1nF TMP36F 5 2 1 VTEMP Figure 58. AD8362 with Temperature Compensation Circuit |
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