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AD8361ARM Datasheet(PDF) 14 Page - Analog Devices |
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AD8361ARM Datasheet(HTML) 14 Page - Analog Devices |
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14 / 16 page ![]() AD8361 –14– REV. A chosen to suit the application. GAIN and VOS are then calculated using the equations: GAIN VV VV OUT OUT IN IN = − () − () 21 21 V V GAIN V OS OUT IN =− × () 11 Both GAIN and VOS drift over temperature. However, the drift of VOS has a bigger influence on the error relative to the output. This can be seen by inserting data from Figures 14 and 17 (con- version gain and intercept drift) into the equation for VOUT. These plots are consistent with Figures 10 and 11 which show that the error due to temperature drift decreases with increasing input level. This results from the offset error having a diminishing influence with increasing level on the overall measurement error. From Figure 14, the average Intercept drift is 0.43 mV/ °C from –40 °C to +25°C and 0.17 mV/°C from +25°C to +85°C. For a less rigorous compensation scheme, the average drift over the complete temperature range can be calculated: DRIFT V C VV CC VOS / .. ° () = −− () +° − − ° () 0 010 0 028 85 40 = 0.000304 V/ °C With the drift of VOS included, the equation for VOUT becomes: Table V. Evaluation Board Configuration Options Component Function Default Condition TP1, TP2 Ground and Supply Vector Pins. Not Applicable SW1 Device Enable. When in Position A, the PWDN pin is connected to +VS and SW1 = B the AD8361 is in power-down mode. In Position B, the PWDN pin is grounded, putting the device in operating mode. SW2/SW3 Operating Mode. Selects either Ground Referenced Mode, Internal Reference SW2 = A, SW3 = B Mode or Supply Reference Mode. See Table I for more details. (Ground Reference Mode) C1, R2 Input Coupling. The 75 Ω resistor in position R2 combines with the AD8361’s R2 = 75 Ω (Size 0402) internal input impedance to give a broadband input impedance of around 50 Ω. C1 = 100 pF (Size 0402) For more precise matching at a particular frequency, R2 can be replaced by a different value (see Input Matching and Figure 39). Capacitor C1 ac-couples the input signal and creates a high-pass input filter whose corner frequency is equal to approximately 8 MHz. C1 can be increased for operation at lower frequencies. If resistive attenuation is desired at the input, series resistor R1, which is nominally 0 Ω, can be replaced by an appropriate value. C2, C3, R6 Power Supply Decoupling. The nominal supply decoupling of 0.01 µF and C2 = 0.01 µF (Size 0402) 100 pF. A series inductor or small resistor can be placed in R6 for additional C3 = 100 pF (Size 0402) decoupling. R6 = 0 Ω (Size 0402) C5 Filter Capacitor. The internal 50 pF averaging capacitor can be augmented C5 = 1 nF (Size 0603) by placing a capacitance in C5. C4, R5 Output Loading. Resistors and capacitors can be placed in C4 and R5 to C4 = R5 = Open load test V rms. (Size 0603) V GAIN V V DRIFT TEMP C OUT IN OS VOS =× ()++ × − ° () 25 The equation can be rewritten to yield a temperature compen- sated value for VIN. V V V DRIFT TEMP C GAIN IN OUT OS VOS = −− × − ° () () 25 EVALUATION BOARD Figures 43 and 46 show the schematic of the AD8361 evalua- tion board. Note that uninstalled components are drawn in as dashed. The layout and silkscreen of the component side are shown in Figures 44, 45, 47, and 48. The board is powered by a single supply in the range, 2.7 V to 5.5 V. The power supply is decoupled by 100 pF and 0.01 µF capacitors. Additional decoupling, in the form of a series resistor or inductor in R6, can also be added. Table V details the various configuration options of the evaluation board. |
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