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AN929 Datasheet(PDF) 8 Page - Microchip Technology |
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AN929 Datasheet(HTML) 8 Page - Microchip Technology |
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8 / 22 page ![]() AN929 DS00929A-page 8 2004 Microchip Technology Inc. EMI/ESD Protection EMI and ESD filters function as both a noise filter and a protective device to the circuit on the PCB. An IC input pin should never be connected directly to a remote sensor because EMI or ESD overvoltage failures will likely occur. Ferrite beads, capacitive feed- through filters, RC filters and transient-voltage-sup- pressor (TVS) zener diodes are popular devices that can be used to provide protection for the sensor circuit. Ferrite beads, capacitive feed-through filters and RC filters function as filters and only limit the slew rate of a transient-input voltage. A voltage-clamping device (such as a TVS zener diode) is required to limit the input voltage to a safe value that will not damage the IC amplifier. Though a TVS device is similar to a standard zener diode, they are designed to turn on fast and dissipate a short duration, high-peak energy voltage transient. In contrast, a zener diode is designed to clamp a steady-state voltage for a long duration. In many applications, a combination of different EMI/ ESD filter devices are often used. One option is to use a capacitive feed-through filter that is located inside the connector, in addition to TVS and RC filters which are placed on the PCB board, as shown in Figure 13. Feed-through capacitors are typically mounted on a conductive chassis, with the mechanical mounting forming the ground connection. The noise signal is filtered at the connector before the signal reaches the PCB. The effectiveness of the filter is usually very good because the inductance associated with the ground connection is minimized. The TVS diodes on the PCB ensure that the transient voltage is limited to a safe value, while the RC filters provide additional filtering to the instrumentation amplifier. FIGURE 13: Remote Sensors May Require Multiple EMI Filter Devices. Figure 14 provides the design equations for a RC filter which can be used with differential and instrumentation amplifiers. The RC combinations of R1/C1 and R2/C2 are used to form common mode filters and reduce the noise which is common to both input lines. The com- mon-mode resistors and capacitors should be matched as close as possible and the resistors should have a tolerance of 1% or better, while the capacitors should be at least 5%. Capacitor C3 forms a differential mode filter that attenuates the signal with respect to the differ- ence in the voltage potentials of the two inputs. C3 also compensates for any mismatch of R1/C1 and R2/C2, which is important because the difference in the R/C combinations degrades an amplifier’s CMRR. FIGURE 14: Providing EMI/ESD Overvoltage Protection with Resistors and Capacitors. Fault Detection Capability It is often necessary to identify a failed sensor, especially in remote-sensing applications. Differential amplifiers can be used to implement a Built-In-Test (BIT) circuit that can determine an open or short failure at the sensor. Figure 15 shows circuits that can be used to detect a failed RTD and thermocouple. A logic inverter gate can be used to monitor the voltage divider network of a RTD. Another approach to provide BIT to a sensor is to add pull-up or pull-down resistors, or both, as shown in Figure 15. The typical failure mode of RTDs and thermocouples is an open-circuit failure. Wire wound RTDs are con- structed from a relatively small gauge wire and are prone to vibration failures. Thermocouple wires can also fail due to vibration because the wires get brittle over time when exposed to high temperatures. Also, the voltage at the amplifier inputs resulting from noise can be equal in magnitude to a functional thermocouple. Instrumentation Amplifier Ferrite Bead Equivalent Circuit Feed-through Capacitor TVS Diode Sensor Connector PCB C2 C1 C3 R2 R1 R1 = R2 C1 = C2 C3 >> C1 and C2 Common Mode Filters f-3dB = 1/(2 π R1C1) f-3dB = 1/(2 π R2C2) Differential Mode Filter Instrumentation Amplifier f 3db – 1 2 π R 1 R 2 + () C 1 C 2 × C 1 C 2 + ------------------- C 3 + -------------------------------------------------------------------------- = |
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