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LT1012 Datasheet(PDF) 5 Page - Linear Technology |
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LT1012 Datasheet(HTML) 5 Page - Linear Technology |
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5 / 12 page ![]() 5 LT1025 1025fb same temperature, but temperature gradients exist within IC packages and across PC boards whenever power is dissipated. For this reason, extreme care must be used to ensure that no temperature gradients exist in the vicinity of the thermocouple terminations, the LT1025, or the thermocouple amplifier. If a gradient cannot be eliminated, leads should be positioned isothermally, especially the LT1025 R– and appropriate output pins, the amplifier input pins, and the gain setting resistor leads. An effect to watch for is amplifier offset voltage warm-up drift caused by mismatched thermocouple materials in the wire-bond/ lead system of the IC package. This effect can be as high as tens of microvolts in TO-5 cans with kovar leads. It has nothing to do with the actual offset drift specification of the amplifier and can occur in amplifiers with measured “zero” drift. Warm-up drift is directly proportional to amplifier power dissipation. It can be minimized by avoiding TO-5 cans, using low supply current amplifiers, and by using the lowest possible supply voltages. Finally, it can be accom- modated by calibrating and specifying the system after a five minute warm-up period. Reversing the Polarity of the 10mV/ °C Output The LT1025 can be made to “stand on its head” to achieve a minus 10mV/ °C output point. This is done as shown in Figure 3. The normal output (VO) is grounded and feed- back is established between the ground pin and the positive supply pin by feeding both of them with currents while coupling them with a 6V zener. The ground pin will now be forced by feedback to generate –10mV/ °C as long as the grounded output is supplying a net “source” current into ground. This condition is satisfied by selecting R1 such that the current through R1 (I–) is more than the sum of the LT1025 supply current, the maximum load current (IL), and the minimum zener current (≈ 50µA). R2 is then selected to supply more current than I–. R V AI R VV V VR A L Z 1 300 2 6 1 280 = µ+ = ≈ +µ + – – , –( ) / For ±15V supplies, with IL = 20µA maximum, R1 = 47k and R2 = 15k. Amplifier Considerations Thermocouple amplifiers need very low offset voltage and drift, and fairly low bias current if an input filter is used. The best precision bipolar amplifiers should be used for type J, K, E, and T thermocouples which have Seebeck coeffi- cients of 40 µV/°C to 60µV/°C. In particularly critical appli- cations or for R and S thermocouples (6 µV/°Cto15µV/°C), a chopper-stabilized amplifier is required. Linear Technol- ogy offers three amplifiers specifically tailored for thermo- couple applications. The LTKA0x is a bipolar design with extremely low offset (< 35 µV), low drift (<1.5µV/°C), very low bias current (<1nA), and almost negligible warm-up drift (supply current is ≈400µA). It is very cost effective even when compared with “jellybean” op amps with vastly inferior specifications. For the most demanding applications, the LTC1050 and LTC1052 CMOS chopper-stabilized amplifiers offer 5 µV offset and 0.05 µV/°C drift (even over the full military temperature range). Input bias current is 30pA, and gain is typically 30 million. These amplifiers should be used for R and S thermocouples, especially if no offset adjust- ments can be tolerated, or a large ambient temperature swing is expected. Regardless of amplifier type, it is suggested that for best possible performance, dual-in-line (DIP) packages be used to avoid thermocouple effects in the kovar leads of TO-5 metal can packages if amplifier supply current ex- ceeds 500 µA. These leads can generate both DC and AC offset terms in the presence of thermal gradients in the package and/or external air motion. APPLICATIO S I FOR ATIO Figure 3 R2 15k R1 47k I+ I– V+ (15V) V– (–15V) IL RL VOUT –10mV/ °C D1 VZ ≈ 6V LT1025 • AG03 LT1025 GND VIN VO |
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