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LTC2414IGN Datasheet(PDF) 36 Page - Linear Technology |
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LTC2414IGN Datasheet(HTML) 36 Page - Linear Technology |
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36 / 48 page ![]() LTC2414/LTC2418 36 241418fa BRIDGE APPLICATIONS Typical strain gauge based bridges deliver only 2mV/Volt of excitation. As the maximum reference voltage of the LTC2414/LTC2418 is 5V, remote sensing of applied exci- tation without additional circuitry requires that excitation be limited to 5V. This gives only 10mV full scale input signal, which can be resolved to 1 part in 10000 without averaging. For many solid state sensors, this is still better than the sensor. Averaging 64 samples however reduces the noise level by a factor of eight, bringing the resolving power to 1 part in 80000, comparable to better weighing systems. Hysteresis and creep effects in the load cells are typically much greater than this. Most applications that require strain measurements to this level of accuracy are measuring slowly changing phenomena, hence the time required to average a large number of readings is usually not an issue. For those systems that require accurate measurement of a small incremental change on a signifi- cant tare weight, the lack of history effects in the LTC2400 family is of great benefit. For those applications that cannot be fulfilled by the LTC2414/LTC2418 alone, compensating for error in exter- nal amplification can be done effectively due to the “no latency” feature of the LTC2414/LTC2418. No latency operation allows samples of the amplifier offset and gain to be interleaved with weighing measurements. The use of correlated double sampling allows suppression of 1/f noise, offset and thermocouple effects within the bridge. Correlated double sampling involves alternating the polar- ity of excitation and dealing with the reversal of input polarity mathematically. Alternatively, bridge excitation can be increased to as much as ±10V, if one of several precision attenuation techniques is used to produce a precision divide operation on the reference signal. An- other option is the use of a reference within the 5V input range of the LTC2414/LTC2418 and developing excitation via fixed gain, or LTC1043 based voltage multiplication, along with remote feedback in the excitation amplifiers, as shown in Figures 46 and 47. Figure 41 shows an example of a simple bridge connec- tion. Note that it is suitable for any bridge application where measurement speed is not of the utmost impor- tance. For many applications where large vessels are weighed, the average weight over an extended period of time is of concern and short term weight is not readily determined due to movement of contents, or mechanical resonance. Often, large weighing applications involve load cells located at each load bearing point, the output of which can be summed passively prior to the signal pro- cessing circuitry, actively with amplification prior to the ADC, or can be digitized via multiple ADC channels and summed mathematically. The mathematical summation of the output of multiple LTC2414/LTC2418’s provides the benefit of a root square reduction in noise. The low power consumption of the LTC2414/LTC2418 makes it attractive for multidrop communication schemes where the ADC is located within the load-cell housing. REF+ REF– SDI SCK SDO CS 20 18 17 16 CH0 CH1 GND VCC FO 11 R1 12 350 Ω BRIDGE 21 22 2414/18 F41 15 9 19 LTC2414/ LTC2418 + R2 R1 AND R2 CAN BE USED TO INCREASE TOLERABLE AC COMPONENT ON REF SIGNALS LT1019 0.1 µF 0.1 µF 10 µF Figure 41. Simple Bridge Connection A direct connection to a load cell is perhaps best incorpo- rated into the load-cell body, as minimizing the distance to the sensor largely eliminates the need for protection devices, RFI suppression and wiring. The LTC2414/ LTC2418 exhibits extremely low temperature dependent drift. As a result, exposure to external ambient tempera- ture ranges does not compromise performance. The in- corporation of any amplification considerably compli- cates thermal stability, as input offset voltages and cur- rents, temperature coefficient of gain settling resistors all become factors. APPLICATIO S I FOR ATIO |
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