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LT1025CS8 Datasheet(PDF) 3 Page - Linear Technology |
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LT1025CS8 Datasheet(HTML) 3 Page - Linear Technology |
3 / 12 page 3 LT1025 1025fb TYPICAL PERFOR A CE CHARACTERISTICS 10mV/ °C Output Temperature Error LT1025 10mV/ °C Output Temperature Error LT1025A Supply Current TEMPERATURE TO BE MEASURED T1 T2 Fe Cu Cu CONSTANTAN LT1025 MUST BE LOCATED NEXT TO COLD JUNCTION FOR TEMPERATURE TRACKING VS } LT1025 • AG01 JUNCTION TEMPERATURE ( °C) *ERROR CURVE FACTORS IN THE NONLINEARITY TERM BUILT IN TO THE LT1025. SEE THEORY OF OPERATION IN APPLICATION GUIDE SECTION –50 –10 –8 –4 –2 0 10 4 0 50 75 LT1025 • G01 –6 6 8 2 –25 25 100 125 GUARANTEED LIMITS* LT1025 JUNCTION TEMPERATURE ( °C) *ERROR CURVE FACTORS IN THE NONLINEARITY TERM BUILT IN TO THE LT1025. SEE THEORY OF OPERATION IN APPLICATION GUIDE SECTION –50 –5 –4 –2 –1 0 5 2 0 50 75 LT1025 • G02 –3 3 4 1 –25 25 100 125 GUARANTEED LIMITS* LT1025A SUPPLY VOLTAGE (V) 0 0 20 60 80 100 200 140 10 20 25 LT1025 • G03 40 160 180 120 515 30 35 40 DOES NOT INCLUDE 30 µA PULL-DOWN CURRENT REQUIRED FOR TEMPERATURES BELOW 0 °C TJ = 125°C PIN 4 TIED TO PIN 5 TJ = 25°C TJ = –55°C The LT1025 was designed to be extremely easy to use, but the following ideas and suggestions should be helpful in obtaining the best possible performance and versatility from this new cold junction compensator. Theory of Operation A thermocouple consists of two dissimilar metals joined together. A voltage (Seebeck EMF) will be generated if the two ends of the thermocouple are at different temperatures. In Figure 1, iron and constantan are joined at the temperature measuring point T1. Two additional thermocouple junctions are formed where the iron and constantan connect to ordinary copper wire. For the purposes of this discussion it is assumed that these two junctions are at the same temperature, T2. The Seebeck voltage, VS, is the product of the Seebeck coefficient α, and the temperature difference, T1 – T2; VS = α (T1 – T2). The junctions at T2 are commonly called the cold junction because a common practice is to immerse the T2 junction in 0 °C ice/water slurry to make T2 independent of room temperature variations. Thermocouple tables are based on a cold-junction temperature of 0 °C. To date, IC manufacturers efforts to make microminiature thermos bottles have not been totally successful. There- fore, an electronically simulated cold-junction is required for most applications. The idea is basically to add a temperature dependent voltage to VS such that the voltage sum is the same as if the T2 junction were at a constant 0 °C instead of at room temperature. This voltage source is called a cold junction compensator. Its output is designed to be 0V at 0 °C and have a slope equal to the Seebeck coefficient over the expected range of T2 temperatures. Figure 1 To operate properly, a cold junction compensator must be at exactly the same temperature as the cold junction of the thermocouple (T2). Therefore, it is important to locate the LT1025 physically close to the cold junction with local temperature gradients minimized. If this is not possible, APPLICATIO S I FOR ATIO |
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