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QT1+10G Datasheet(PDF) 7 Page - Quantum Research Group |
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QT1+10G Datasheet(HTML) 7 Page - Quantum Research Group |
7 / 12 page should be placed very close to the device’s power pins. Without this capacitor the part can break into high frequency oscillation, get physically hot, stop working, or become damaged. PCB Cleanliness: All capacitive sensors should be treated as highly sensitive circuits which can be influenced by stray conductive leakage paths. QT devices have a basic resolution in the femtofarad range; in this region, there is no such thing as ‘no clean flux’. Flux absorbs moisture and becomes conductive between solder joints, causing signal drift and resultant false detections or temporary loss of sensitivity. Conformal coatings will trap in existing amounts of moisture which will then become highly temperature sensitive. The designer should strongly consider ultrasonic cleaning as part of the manufacturing process, and in more extreme cases, the use of conformal coatings after cleaning and baking. 3.3.1 SUPPLY CURRENT Measuring average power consumption is a challenging task due to the burst nature of the device’s operation. Even a good quality RMS DMM will have difficulty tracking the relatively slow burst rate, and will show erratic readings. The easiest way to measure Idd is to put a very large capacitor, such as 2,700µF across the power pins, and put a 220 ohm resistor from there back to the power source. Measure the voltage across the 220 resistor with a DMM and compute the current based on Ohm’s law. This circuit will average out current to provide a much smoother reading. To reduce the current consumption the most, use high or low gain pin settings only, the smallest value of Cs possible that works, and a 470K resistor (Rs) across Cs (Figure 1-1). Rs acts to help discharge capacitor Cs between bursts, and its presence substantially reduces power consumption. 3.3.2 ESD PROTECTION In cases where the electrode is placed behind a dielectric panel, the IC will be protected from direct static discharge. However even with a panel transients can still flow into the electrode via induction, or in extreme cases via dielectric breakdown. Porous materials may allow a spark to tunnel right through the material. Testing is required to reveal any problems. The device has diode protection on its terminals which will absorb and protect the device from most ESD events; the usefulness of the internal clamping will depending on the dielectric properties, panel thickness, and rise time of the ESD transients. The best method available to suppress ESD and RFI is to insert a series resistor Re in series with the electrode as shown in Figure 1-1. The value should be the largest that does not affect sensing performance. If Re is too high, the gain of the sensor will decrease. Because the charge and transfer times of the QT110 are relatively long (~2µs), the circuit can tolerate a large value of Re, often more than 10k ohms in most cases. Diodes or semiconductor transient protection devices or MOV's on the electrode trace are not advised; these devices have extremely large amounts of nonlinear parasitic capacitance which will swamp the capacitance of the electrode and cause false detections and other forms of instability. Diodes also act as RF detectors and will cause serious RF immunity problems. 3.4 EMC AND RELATED NOISE ISSUES External AC fields (EMI) due to RF transmitters or electrical noise sources can cause false detections or unexplained shifts in sensitivity. The influence of external fields on the sensor is reduced by means of the Rseries described in Section 3.2. The Cs capacitor and Rseries (Figure 1-1) form a natural low-pass filter for incoming RF signals; the roll-off frequency of this network is defined by - FR = 1 2 ✜RseriesCs If for example Cs = 22nF, and Rseries = 10K ohms, the rolloff frequency to EMI is 723Hz, vastly lower than any credible external noise source (except for mains frequencies i.e. 50 / 60 Hz). However, Rseries and Cs must both be placed very close to the body of the IC so that the lead lengths between them and the IC do not form an unfiltered antenna at very high frequencies. PCB layout, grounding, and the structure of the input circuitry have a great bearing on the success of a design to withstand electromagnetic fields and be relatively noise-free. These design rules should be adhered to for best ESD and EMC results: 1. Use only SMT components. 2. Keep Cs, Rs, Re and Vdd bypass cap close to the IC. 3. Maximize Re to the limit where sensitivity is not affected. 4. Do not place the electrode or its connecting trace near other traces, or near a ground plane. 5. Do use a ground plane under and around the QT110 itself, back to the regulator and power connector (but not beyond the Cs capacitor). 6. Do not place an electrode (or its wiring) of one QT11x device near the electrode or wiring of another device, to prevent cross interference. 7. Keep the electrode (and its wiring) away from other traces carrying AC or switched signals. 8. If there are LEDs or LED wiring near the electrode or its wiring (ie for backlighting of the key), bypass the LED wiring to ground on both its ends. 9. Use a voltage regulator just for the QT110 to eliminate noise coupling from other switching sources via Vdd. Make sure the regulator’s transient load stability provides for a stable voltage just before each burst commences. For further tips on construction, PCB design, and EMC issues browse the application notes and faq at www.qprox.com LQ 7 QT110 R1.04/0405 |
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