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QT113 Datasheet(PDF) 6 Page - Quantum Research Group |
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QT113 Datasheet(HTML) 6 Page - Quantum Research Group |
6 / 12 page induce detection ‘cycling’, whereby an object is detected, the load is turned on, the supply sags, the detection is no longer sensed, the load is turned off, the supply rises and the object is reacquired, ad infinitum. To prevent this occurrence, the output should only be lightly loaded if the device is operated from an unregulated supply, e.g. batteries. Detection ‘stiction’, the opposite effect, can occur if a load is shed when Out is active. The output of the QT113 can directly drive a resistively limited LED. The LED should be connected with its cathode to the output and its anode towards Vcc, so that it lights when the sensor is active. If desired the LED can be connected from Out to ground, and driven on when the sensor is inactive. 3 - CIRCUIT GUIDELINES 3.1 SAMPLE CAPACITOR Charge sampler Cs can be virtually any plastic film or medium-K ceramic capacitor. The acceptable Cs range is from 10nF to 500nF depending on the sensitivity required; larger values of Cs demand higher stability to ensure reliable sensing. Acceptable capacitor types include PPS film, polypropylene film, NPO/C0G ceramic, and X7R ceramic. 3.2 OPTION STRAPPING The option pins Opt1 and Opt2 should never be left floating. If they are floated, the device will draw excess power and the options will not be properly read on powerup. Intentionally, there are no pullup resistors on these lines, since pullup resistors add to power drain if tied low. The Gain input should be connected to either Vdd or Gnd. Tables 1-1 and 2-1 show the option strap configurations available. 3.4 POWER SUPPLY, PCB LAYOUT The power supply can range from 2.5 to 5.0 volts. At 3 volts current drain averages less than 600µA in most cases, but can be higher if Cs is large. Increasing Cx values will actually decrease power drain. Operation can be from batteries, but be cautious about loads causing supply droop (see Output Drive, Section 2.2.4). As battery voltage sags with use or fluctuates slowly with temperature, the QT113 will track and compensate for these changes automatically with only minor changes in sensitivity. If the power supply is shared with another electronic system, care should be taken to assure that the supply is free of digital spikes, sags, and surges which can adversely affect the QT113. The QT113 will track slow changes in Vdd, but it can be affected by rapid voltage steps. if desired, the supply can be regulated using a conventional low current regulator, for example CMOS regulators that have low quiescent currents. Bear in mind that such regulators generally have very poor transient line and load stability; in some cases, shunting Vdd to Vss with a 4.7K resistor to induce a continuous current drain can have a very positive effect on regulator performance. Parts placement: The chip should be placed to minimize the SNS2 trace length to reduce low frequency pickup, and to reduce stray Cx which degrades gain. The Cs and Rseries resistors (see Figure 1-1) should be placed as close to the body of the chip as possible so that the SNS2 trace between Rseries and the SNS2 pin is very short, thereby reducing the antenna-like ability of this trace to pick up high frequency signals and feed them directly into the chip. For best EMC performance the circuit should be made entirely with SMT components. SNS trace routing: Keep the SNS2 electrode trace (and the electrode itself) away from other signal, power, and ground traces including over or next to ground planes. Adjacent switching signals can induce noise onto the sensing signal; lQ 6 R1.05/0405 Figure 2-4 Using a micro to obtain HB pulses in either output state Figure 2-3 Getting HearBeat pulses with a pull-down resistor 3 46 5 1 +2.5 to 5 7 2 OUT OPT1 OPT2 GA IN SNS1 SNS2 Vss Vdd 8 Ro H eartBeat™ P u lses Microcontroller PORT_M.x PORT_M.y 3 46 5 7 2 OUT OPT1 OPT2 GAIN SNS1 SNS2 Ro Figure 2-5 Eliminating HB Pulses 3 46 5 7 2 OUT OPT1 OPT2 GAIN SNS1 SNS2 CM O S 100pF Co GATE OR MICRO INPU T |
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