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AD8571ARM Datasheet(PDF) 12 Page - Analog Devices |
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AD8571ARM Datasheet(HTML) 12 Page - Analog Devices |
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12 / 19 page ![]() AD8571/AD8572/AD8574 –12– REV. 0 VOUT VIN AD8572 VOUT VIN AD8572 VOUT VIN AD8572 Figure 46. Guard Ring Layout and Connections to Reduce PC Board Leakage Currents V V+ VREF VIN1 VIN2 GUARD RING R2 R2 R1 R1 AD8572 VREF GUARD RING Figure 47. Top View of AD8572 SOIC Layout with Guard Rings Other potential sources of offset error are thermoelectric voltages on the circuit board. This voltage, also called Seebeck voltage, occurs at the junction of two dissimilar metals and is proportional to the temperature of the junction. The most common metallic junctions on a circuit board are solder-to-board trace and solder- to-component lead. Figure 48 shows a cross-section diagram view of the thermal voltage error sources. If the temperature of the PC board at one end of the component (TA1) is different from the temperature at the other end (TA2), the Seebeck voltages will not be equal, resulting in a thermal voltage error. This thermocouple error can be reduced by using dummy com- ponents to match the thermoelectric error source. Placing the dummy component as close as possible to its partner will ensure both Seebeck voltages are equal, thus canceling the thermo- couple error. Maintaining a constant ambient temperature on the circuit board will further reduce this error. The use of a ground plane will help distribute heat throughout the board and will also reduce EMI noise pickup. SURFACE MOUNT COMPONENT COMPONENT LEAD SOLDER PC BOARD COPPER TRACE VSC2 + + VTS2 TA2 TA1 VSC1 + + VTS1 IF TA1 = TA2, THEN VTS1 + VSC1 = VTS2 + VSC2 Figure 48. Mismatch in Seebeck Voltages Causes a Thermoelectric Voltage Error VOUT VIN AD857x AV = 1 + (RF /R1) R1 RF RS = R1 NOTE: RS SHOULD BE PLACED IN CLOSE PROXIMITY AND ALIGNMENT TO R1 TO BALANCE SEEBECK VOLTAGES Figure 49. Using Dummy Components to Cancel Thermoelectric Voltage Errors 1/f Noise Characteristics Another advantage of autozero amplifiers is their ability to cancel flicker noise. Flicker noise, also known as 1/f noise, is noise inher- ent in the physics of semiconductor devices and increases 3 dB for every octave decrease in frequency. The 1/f corner frequency of an amplifier is the frequency at which the flicker noise is equal to the broadband noise of the amplifier. At lower frequencies, flicker noise dominates, causing higher degrees of error for sub- Hertz frequencies or dc precision applications. Because the AD857x amplifiers are self-correcting op amps, they do not have increasing flicker noise at lower frequencies. In essence, low frequency noise is treated as a slowly varying offset error and is greatly reduced as a result of autocorrection. The correction becomes more effective as the noise frequency approaches dc, offsetting the tendency of the noise to increase exponentially as frequency decreases. This allows the AD857x to have lower noise near dc than standard low-noise amplifiers that are susceptible to 1/f noise. Random Autozero Correction Eliminates Intermodulation Distortion The AD857x can be used as a conventional op amp for gains up to 1 MHz. The autozero correction frequency of the device continuously varies, based on a pseudo-random generator with a uniform distribution from 2 kHz to 4 kHz. The randomization of the autocorrection clock creates a continuous randomization of intermodulation distortion (IMD) products, which show up as simple broadband noise at the output of the amplifier. This noise naturally combines with the amplifier’s voltage noise in a root-squared-sum fashion, resulting in an output free of IMD. Figure 50a shows the spectral output of an AD8572 with the amplifier configured for unity gain and the input grounded. Figure 50b shows the spectral output with the amplifier configured for a gain of 60 dB. |
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